MESSENGER:
Software Interface Specification for the
Calibrated Data Records of the Energetic Particle and Plasma Spectrometer
Version 1J
Lillian Nguyen
Johns Hopkins
University Applied Physics Laboratory
Document Review
This document and the archive it describes have been through PDS Peer Review and have been accepted into the PDS archive.
George Ho, MESSENGER EPPS Instrument Scientist, has reviewed and approved this document.
Jim Raines, MESSENGER FIPS Instrument Engineer, has reviewed and approved this document.
Steve Joy, PDS PPI Node Representative, has reviewed and approved this document.
Susan Ensor, MESSENGER Science
Operations Center Lead, has reviewed and approved this document.
Table
of Contents
1 Purpose and Scope of Document..................................................................................... 6
1.1 Purpose................................................................................................................................. 6
1.2 Scope.................................................................................................................................... 6
2 Applicable Documents....................................................................................................... 6
3 Relationships with Other Interfaces......................................................................... 7
4 Roles and Responsibilities............................................................................................... 7
5 Data Product Characteristics and Environment..................................................... 7
5.1 Instrument Overview............................................................................................................ 7
5.1.1 FIPS Overview................................................................................................................... 8
5.1.2 EPS Overview.................................................................................................................... 9
5.2 Data Product Overview...................................................................................................... 12
5.2.1 EPS Data Products........................................................................................................... 12
5.2.2 FIPS Data Products.......................................................................................................... 22
5.3 Data Processing.................................................................................................................. 28
5.3.1 Data Processing Level....................................................................................................... 28
5.3.2 Data Product Generation................................................................................................... 28
5.3.3 Data Flow...................................................................................................................... 29
5.3.4 Labeling and Identification................................................................................................ 31
5.4 Standards Used in Generating Data Products..................................................................... 45
5.4.1 PDS Standards................................................................................................................ 45
5.4.2 Time Standards................................................................................................................ 45
5.4.3 Coordinate Systems.......................................................................................................... 46
5.4.4 Data Storage Conventions................................................................................................. 47
5.5 Data Validation................................................................................................................. 47
6 Detailed Data Product Specification......................................................................... 48
6.1 Data Product Structure and Organization........................................................................ 48
6.2 Handling Errors................................................................................................................. 49
6.3 Data Format Description..................................................................................................... 49
6.4 Label and Header Descriptions............................................................................................ 49
6.5 File Naming Conventions.................................................................................................... 52
6.6 Archive Volume and File Size.............................................................................................. 53
6.7 Directory Structure and Contents for EPPS
Documentation Volume................................. 53
6.7.1 Directory Contents........................................................................................................... 54
6.8 Directory Structure and Contents for EPPS Data Volume................................................. 55
6.8.1 Directory Contents........................................................................................................... 55
7 Archive Release Schedule to PDS................................................................................ 57
8 Appendices............................................................................................................................. 57
8.1 EPSHIGH_CDR.FMT Table Columns.................................................................................... 57
8.2 EPSMED_CDR.FMT Table Columns..................................................................................... 65
8.3 EPS_PHA_CDR.FMT Table Columns.................................................................................... 73
8.4 EPS_HIRES_CDR.FMT Table Columns................................................................................. 76
8.5 EPS_LORES_CDR.FMT Table Columns................................................................................ 79
8.6 EPS_SUM_CDR.FMT Table Columns................................................................................... 83
8.7 EPS_SCAN_CDR.FMT Table Columns................................................................................. 84
8.8 FIPS_HI_CDR.FMT Table Columns...................................................................................... 88
8.9 FIPS_MED_CDR.FMT Table Columns.................................................................................. 89
8.10 FIPS_PHA_CDR.FMT Table Columns................................................................................. 90
8.11 FIPS_SCAN_CDR.FMT Table Columns............................................................................... 90
8.12 FIPS_HRPVD_CDR.FMT Table Columns............................................................................ 90
8.13 FIPS_EQ.FMT Table Columns............................................................................................ 90
8.14 FIPS_FOVPIXEL.FMT Table Columns................................................................................ 90
8.15 SPICE Kernel Files Used in MESSENGER Data
Products.................................................... 90
8.16 CODMAC/NASA Definition of Processing
Levels................................................................ 90
8.17 MESSENGER Glossary and Acronym List........................................................................... 90
Table 1 Revision History
|
Version |
Author |
Date |
Description |
Sections |
|
1A |
L. Nguyen |
7/1/2009 |
Initial
revision |
All |
|
1B |
L. Nguyen |
12/3/2009 |
Addresses
issues from first PDS review. Document
changes for FSW7. |
2, 3, 5, 6, 8 |
|
Add to description of EPS
collimator |
5.1.2.3 |
|||
|
Document EPS data product
changes |
5.2.1, inc.
table 2 |
|||
|
Add and update sample
labels |
5.3.4 |
|||
|
Add S/C event time format |
5.4.2 |
|||
|
Update PDS archive
directory structures |
6.7, 6.8 |
|||
|
Add section for FIPS
efficiency ancillary data |
8.14 |
|||
|
1C |
L. Nguyen |
1/6/2010 |
Minor changes
after PDS re-review |
various |
|
1D |
M.
Reid |
1/7/2010 |
Minor
additions of missing files |
6.7, 6.8 |
|
1E |
J.
Raines |
1/18/2010 |
Add
explanation of unexpected features in EPS data due to TOF issues and negative
values in SCAN mode data |
5.2.1.1 |
|
Add
explanation of criteria for PHA event processing |
5.2.1.2 |
|||
|
Change “flux”
to “differential intensity” and “velocity” to “normalized velocity”. |
5, 8, tables 15-18 |
|||
|
Add
description of S/C blocking of FIPS FOV |
5.2.2.1 |
|||
|
Add to
description of PHA data velocity distribution. |
5.2.2.3 |
|||
|
Remove
5.3.4.1.4 FIPS Efficiency Table PDS Label and format table |
5.3.4.1.4, 8.15 |
|||
|
1F |
M. Reid |
2/5/2010 |
Updated name
on signature page; regenerated TOC. |
|
|
1G |
S. Ensor |
6/16/2011 |
Replaced
signature page with document review info. |
|
|
1H |
S.Ensor |
5/26/2012 |
Change [2]
from Data Management and Science
Analysis Plan to Data Management
and Archiving Plan. |
2 |
|
1I |
M. Reid |
7/15/2014 |
Added
descriptions of the FIPS Field Of View ancillary/calibration products.
Updated document volume directory structure description. |
5.2.2.4, 5.3.4.14, 6.5,
6.7, 8.14 |
|
1J |
M. Reid |
7/22/2014 |
Minor mods to
FIPA_F*.LBL example. Included the INDEX directory in the documentation volume
description. |
5.3.4.14. 6.7 |
Table 2 To Be Determined (TBD) Items
|
Location |
Description |
|
SIS §6.6 |
Data archive
size |
This document will serve to
provide users of the MErcury Surface, Space ENvironment, GEochemistry, and
Ranging (MESSENGER) Energetic Particle and Plasma Spectrometer (EPPS) data
products with a detailed description of the EPPS instrument, data product
generation, validation and storage. Note
that the EPPS is made up of two instrument subsystems, the Fast Imaging Plasma
Spectrometer (FIPS), and the Energetic Particle Spectrometer (EPS). The FIPS and EPS will be described in
individual sections within this document. They will be referred to separately
when necessary and referred to as the EPPS instrument when dealing with areas
common to both instruments. The FIPS
covers the lower energy range of particles and measures the mass per charge
(M/Q), energy per charge (E/Q) and incoming direction of each charged particle.
The EPS covers the higher energy range and measures mass, energy, and incoming
direction of each particle. The MESSENGER EPPS data products are deliverables
to the Planetary Data System (PDS) and the scientific community that it
supports. All data formats are based on the PDS standard.
The EPPS science data are divided into two categories:
Level 2 edited-raw data (referred to as Experiment Data Records or EDRs) and
processed data (referred to as reduced data records or RDRs). RDRs are
generated from EDRs, and represent data calibrated to a physical unit such as
particle intensity (Level 3), resampled Level 4 data products, or derived Level
5 data products. RDRs consist of Calibrated Data Records (CDRs), Derived Data
Products (DDP) and Derived Analysis Products (DAP). This SIS
describes the EPPS CDR data products.
CDRs consist of processed spectra and pulse-height
analysis (PHA) data, including a description of the observation geometry. The
CDR data will be delivered to the PDS as CODMAC Level 3 data. EPPS’s CDR is
formatted to include standard PDS labels. A detailed description of all data
products in the EPPS’s CDR follows.
In addition this SIS describes the
EPPS documentation volume, which will contain products related to both the EDR
and CDR level archives. The contents of the documentation volume will enable
one to conduct useful analysis of the CDRs. The documentation volume is
described in greater detail in section 6.6.
The MESSENGER EPPS SIS is
responsive to the following Documents:
1.
Planetary Data
System Standards Reference, Feb 27, 2009, Version 3.8. JPL D-7669, Part-2.
3.
MESSENGER Project
Archive Generation, Validation, and Distribution Plan
4.
MESSENGER Mercury:
Surface, Space Environment, Geochemistry, Ranging; A mission to Orbit and
Explore the Planet Mercury, Concept Study, March 1999. Document ID
number FG632/ 99-0479
5.
[PLR] Appendix 7
to the discovery program Plan; Program Level Requirement for the MESSENGER
Discovery project; June 20, 2001.
The following
documents may be referenced for details on the EPPS instruments:
7.
Zurbuchen
et al. (The Fast Ion Plasma Spectrometer (FIPS) calibration report, MESSENGER
Project report, 2004)
The EPPS CDR data products are stored at the Science Operations Center (SOC). The data products will be electronically transferred to the PDS Planetary Plasma Interactions (PPI) Node according to the delivery schedule in [2]. The data in the CDR files will be stored in PDS ASCII TABLE objects unless stated otherwise (section 5.2).
Due to changes in the EPPS instrument flight software, the EPS and FIPS CDR data products contain both pre- and post- flight software change formats. The flight software (FSW) changes affecting EPPS are version 5 (FSW5), version 6 (FSW6), and version 7 (FSW7). FSW5 was uploaded on 9/6/2007, and FSW6 was uploaded on 8/18/2008 and implemented a day later. FSW7 was uploaded on 8/18/2009. The following sections detail the effects of the flight software changes on the CDR data products.
The roles and responsibilities of the instrument teams,
Applied Physics Lab (APL), Applied Coherent Technology (ACT), and the Planetary
Data System (PDS) are discussed in sections 5.3.2
and 5.3.3.
The EPPS
system encompasses two instrument subsystems – the Energetic Particle
Spectrometer (EPS) and the Fast Imaging Plasma Spectrometer (FIPS). EPS covers
the energy range of 25 to >500 keV for electrons, and 10 keV/nucleon to ~3
MeV total energy for ions. FIPS covers
the energy/charge range of <50 eV/q to 20 keV/q. The Johns Hopkins University/Applied Physics
Laboratory constructed the EPS instrument.
It provides electron, high and low-energy ion as well as diagnostic
events as a single stream of data that is placed into the EPS event FIFO (First In, First out) for processing by the EPPS flight
software. The FIPS instrument was constructed by the University of Michigan
Space Physics Research Laboratory. It
provides a single serial stream of event data to the EPPS system at rates of up
to 50K events/sec. The desired throughput for FIPS charged particle event
processing as well as for EPS event processing is 5 kHz. FIPS generates a
single 48-bit raw event packet format which includes a 1-bit header that
identifies the event as a proton event or a non-proton event; an 11-bit
time-of-flight (TOF) value; as well as a Wedge, Strip and ZigZag values (each
12 bits in size). In addition, the FIPS system generates counter and
housekeeping information that the EPPS software can access via the Inter-Integrated Circuit
(I2C) bus interface. Detailed
descriptions of the EPS and FIPS sensor can be found, respectively, in Livi et
al. (The energetic particle spectrometer (EPS) on MESSENGER: Instrument
description, characterization, and calibration, MESSENGER Project report, 2004)
and Zurbuchen et al. (The Fast Ion Plasma Spectrometer (FIPS) calibration
report, MESSENGER Project report, 2004).
The Fast Imaging Plasma
Spectrometer (FIPS) sensor measures the energy per charge (E/q), time-of-flight
(TOF) and incident angles for plasma ions entering the sensor. Intensities, velocity distributions and mass
per charge (m/q) distributions are derived from these measurements and make up
FIPS primary science data. This data
will be used to understand the kinetic properties, angular distributions and
composition of Mercury magnetospheric ions as well as contribute to the
characterization of the planetary magnetic field.
Ions measured by FIPS pass through
an electrostatic analyzer (ESA), located at the entrance to the sensor, a post
acceleration chamber between the output of the ESA and the carbon foil, and a
time-of-flight telescope. The ESA at the
entrance to FIPS acts as a wide-angle lens for ions, with a 1.4 sr field of view.
It only allows ions with a specific E/q band to enter through its output
plane. This band is stepped through 64
values to complete one measurement cycle (scan), nominally from 0.046-13.3
keV/e. FIPS is normally operated in one
of two stepping rates, once step per second (normal mode) or one step per 100
milliseconds (burst mode). When delays
due to high voltage ramp-ups are included, these result in cycle times of 64
sec and 8 sec, respectively. The
operation of FIPS is highly configurable via table upload. The time spent in each step can, in
principal, be set to arbitrary values, different for each step. Associated with each E/q step is a deflection
voltage setting, a threshold, a settling time, and an integration (dwell) time.
Ions exit the output plane of the
ESA and are then accelerated in the post acceleration chamber. This acceleration is done to give low energy
ions sufficient energy to penetrate the carbon foil. The acceleration also helps to reduce energy
straggling and angular scattering – effects that cause degradation in mass
resolution and imaging. When ions exit
the carbon foil, secondary electrons are liberated. These electrons travel to the Start MCP
(microchannel plate), providing a timing-start signal and incident angle
information via impact location on a position-sensing anode. The ion then
travels through the TOF chamber and strikes the Stop MCP, providing a
timing-stop signal and allowing computation of TOF. From E/q and TOF, m/q can be computed. FIPS can measure species from H to Fe, 1-60
amu/e (or higher).
Details of FIPS operations can be
found in [8].
EPS is a compact TOF telescope with two main components: a TOF section and a Solid State Detectors (SSD) array. The SSD comprises six ion implanted planar silicon detectors, each with four pixel, two dedicated to ion measurements and two to electron measurements; for a total of 24 SSD elements. Particles enter the system through a mechanical collimator that delimits the look direction into the instrument. Particles that pass through the collimator will then transit through a thin composite Start foil (Polyimide + Aluminum, 10 mg/cm2) and onto the TOF region of the instrument.
Electrons are released from the inner surface of the Start foil and focused to a well-defined region on a microchannel plate (MCP) to generate the START signal in a dedicated anode. The incident ions are not significantly affected by the electric fields of the focusing optics. After 6 cm flight path, ions traverse the Stop foil, which is a Polyimide + Palladium (19 mg/cm2) composite foil. The secondary electrons released by the stop foil are steered to the MCP and generate the STOP signal. Electron trajectory simulations show that there is less then 2 ns dispersion in the transit time of the secondary electron from the foil to the MCP. Sub-nanosecond dispersion is required so as not to misidentify ion species. If we get both a START and STOP signal (double coincidence), then we can obtain the time, t, for the particle to travel a known distance (d=6 cm). For triple coincidence we must have the START, STOP and energy measured (Emeas) by the SSDs. Using these measured parameters, we can calculate the mass (M), and the incident energy (E) of each ion using the following equations:
Emeas takes into account the small energy loss of the ions passing through the front, start and stop foils, and g is a number less than one that takes into account the energy loss and pulse height defect in the SSDs. EToF takes into account the even smaller energy loss or gain (b) in the front and start foils, and may also include up to ~2.5 keV electrostatic pre-acceleration of ions that remain charged on exiting the “front” foil. If the energy of the incident particle is not large enough to trigger the SSD such that only t is measured, then the pulse height of the start anode will be used to discriminate whether it is a light (M~1 amu), or heavy (M > 1 amu) ion. At the same value of TOF, heavy ions have been shown to generate substantially more secondary electrons than do protons.
Besides composition measurements, the particle’s angular direction can be determined. The pair of start and stop anodes provide the polar entrance angle of the incident particle. The polar angle of +80º to -80º is divided into six equal sectors (nominally 27º).
Energetic electrons have higher penetration power than ions at the same energy. The SSDs dedicated to electron detection in EPS are covered by a thin layer (flashing) of 1mm of Aluminum. This dead layer stops protons with energy less then ~250 keV; on the other hand electrons lose less than 10 keV energy by the interaction with this dead layer. Electrons are identified in EPS by the presence of an energy signal. The TOF spectra collected in the adjacent SSD (without flashing) will be used during ground data analysis for checking and correcting for the proton contamination.
“Calibration” for a particle instrument like EPS means determining the following:
All these functions need to be characterized and the relevant parameters need to be determined before flight.
Flux,
differential intensity and phase space density
The number of particles N that traverse an area A during a time t can be characterized by the Flux F [1/cm2/s]
N= A * t * F
or by the Intensity I [1/cm2/s/sr]
N= A * t * ò I
cos(û) dW
where W is solid angle and û is angle to the area normal. Here, the geometric characteristics of the sensor determine the limits on the integration.
Often used is the quantity differential intensity f [1/cm2/s/sr/keV], defined as the number of particles with energy between E and E+ΔE that traverse the area A during the time t, where
N(E)=f(E) * A * t * DW *
ΔE
In three dimensions, with θ being the polar angle and φ the azimuthal angle of a polar reference system:
d3N(E,θ,φ)=f(E,
θ, φ) * A cos(û) * t * dE cos θ dθ dφ
note that f(E, θ, φ) is related to the phase space density psd (number of particles in the configuration space element d3R and with velocity between v and v+ d3v) by the simple relationship in the non-relativistic limit (valid for ions measured by EPS but not for the higher energy electrons):
psd(s3/ cm6)=f(1/cm2/s/sr/keV)
* m/v2
For relativistic particles one generally utilizes momentum space rather than velocity space, and the corresponding expression is:
psd(s3/gm.cm6)
= f(1/cm2/s/sr/keV) / p2
Where “p” is momentum.
Definition of sensor
transfer function and geometric factor
The number of counts N of particles of mass m, in the energy band around mean energy E, angular band Δθ around mean polar direction θ, and angular band Δφ around the mean azimuthal direction φ, measured by the instrument during the time δt can be expressed as:
N(E, θ, φ; m) = δt * òΔE òΔθ
òΔφ f(E, θ, φ; m) * A cos(û) * dE cos
θ dθ dφ
If f(E, θ, φ) is a Dirac δ function (monoenergetic, infinitely narrow beam), then
N(E, θ, φ; m) = δt * f(E, θ, φ; m) * G(E,
θ, φ; m)
Where G(E, θ, φ; m) [cm2 sr keV] is the transfer function of the instrument.
In the other limit, when the flux is completely isotropic (all directions the same)
N(E; m) = δt * f(E; m) *
GF(E; m)
GF is called geometric factor and represent a measure of the efficiency of the system (count rate/flux), and typically is a function of energy and species.
The goal of the calibration is to characterize the function G(E, θ, φ; m), so that from measurements of the count rates it is possible to constrain f(E, θ, φ; m). Note that an exact inversion of the integral is rarely possible, and we can compute only the coefficients of some tailored expansion of f(E, θ, φ; m), like for example in spherical harmonics (Legendre polynomials). The accuracy of these coefficients depends on both the raster coverage of the measurements and on the calibration.
The EPS collimator consists of four concentric half circular plates that have holes aligned with a common point of origin at the center of the EPS TOF telescope. The size and number of collimator holes define the geometric factor GF of the instrument. The many-holes collimator design minimizes the scattering of ions and electrons at the collimator while restricting the field-of-view (FOV) of the instrument.
GEANT4 simulation shows that the geometry factor for the total SSD area to be 0.016 cm2 sr. The simulation accounted for gaps between the detectors, but did not allow for the guard ring dead area between the large and small pixels or the losses in the two grids used to mount the thin foils. Hence, before grid losses, the total large pixel geometry factor is therefore GFSSD = 0.0152 cm2 sr, and the small pixels would be 0.0008 cm2 sr. The grid losses are actual blockages, so these should be included in the geometry factor. EPS used 40 lines per inch grids on the foils that are 86% transmissive. Therefore, for the 12 large pixels, we have a total geometry factor of 0.862x0.0152, or 0.011 cm2 sr, and each large pixel will be 1/12 of that, or GFSSD-Large = 0.001 cm2 sr. For the 12 small pixels, we have a total geometry factor of 5.6x10-4 cm2 sr, or GFSSD-Small = 4.7x10-5 cm2 sr per pixel. The current simulation does not model the scattering of low energy ion and electron in the collimator, hence the current value of GFSSD is constant with energy and look direction. The instrument team may revise the value of GFSSD at a later time when we develop a further understanding of the instrument response as a function of direction, energy and species.
GFTOF for the Low Energy Ions (TOF-only) is roughly twice the SSD values, or ~0.03 cm2 sr. Note that the needed Transfer Factor G depends also on the counting efficiency ekj which depends, in turn, on species and instrument mode. However, these values were never conclusively determined. During the time of instrument check out shortly after launch, EPS’s TOF section suffered a failure; subsequently, EPS lost its ability to measure ions by elemental mass species. All in-flight EPS data contains null TOF values, hence, EPS can now only measure
N(E) = δt * f(E) * GFSSD
GFSSD is now the geometric factor and represent a measure of the efficiency of the system (count rate/flux), and is constant with look direction, energy and species. This is the standard approximate conversion of count rate to intensity assuming the channel efficiency is part of the geometry factor. The shape of the energy spectrum will also affect the response.
The CDR data products generated by the EPS and FIPS subsystems are described in this section. For all of the CDR products there is a detached PDS label file which describes the contents of one data file. Each label file will have the same base name as the data file it is describing, with the extension “.LBL” to denote a label file. The label file defines the start time and end of the observation, product creation time, and the structure of the ASCII tables. Each data file contains the data collected on a given earth day.
The EPS portion of the data archive will consist of seven CDR data products, which are in direct correspondence to the EPS EDR products. However, the spectra and PHA data are converted to physical units instead of instrument engineering units. The EPS instrument creates all of its different science data packets during one observation, but the packets are telemetered to the ground at different times based on priority. The different formats of these data packets do not lend themselves to standardization into one CDR file format. For example, the high priority science data packet contains the EPS high priority spectra, housekeeping information, and PHA data. Therefore, different CDR formats have been developed, each of which captures one specific data grouping – spectra, housekeeping information, or PHA data. A given CDR data file will contain all the observations obtained on the same earth day. Table 3 shows the different EPS data products and their files. Each data product is identified within the PDS label by a STANDARD_DATA_PRODUCT_ID value (shown in parentheses).
Table 3 EPS Data
Products
|
Data Product |
Product Description |
|
· Spectra Data – contains spectral data, hardware and software rate counters in ASCII table format. Data and counter values are taken from the High Priority (order that they download to ground) Science Packet |
|
|
·
Spectra data – contains spectral data, hardware and software
rate counters in ASCII table format. Data and counter values are taken from
the Medium Priority (order that they download to ground) Science Packet. |
|
|
·
PHA Data – contains Pulse Height Analysis data in ASCII table
format. The PHA data product is generated from the high, medium, or low
priority science packet. The priority level will be identified within the PDS
label. ·
As of 8/18/2008 the PHA data product is generated from PHA data
packets. There is no priority level associated with the PHA CDR since the
high, medium, and low priority packets are retired on 8/18/2008. |
|
|
·
Data file – high-res (energy channels) ion and electron energy
spectra |
|
|
·
Data file – lo-res (energy channels) ion and electron energy
spectra and rate counters. |
|
|
·
PDS label file – describes the data product and contains
pointers to the data file: ·
Data file – Contains a subset of rate counters and low
resolution energy spectra |
|
|
·
PDS label file – describes the data product and contains
pointers to the data file: ·
Data file – Contains the integrated hardware counters over four
energy thresholds. Each threshold setting and integration lasts ¼ second. |
An EPS data quality flag represents the daily status of the scientific quality of the EPS data. When EPS is configured to take nominal science data for that entire day of operation, the flag is set to 0. On the contrary, when EPS is not properly configured to take nominal science data (i.e. initial turn-on, thresholds are not set, etc) during anytime in that particular day, the data quality flag is set to 1. When that happens, users of the EPS data are advised to contact the EPS team for further explanation of the available data during that day. The data quality is specified in the NOTE section of the PDS label for a given data file.
A value of -1.0e-38 in any ASCII Real field means that value is invalid (or not applicable).
The EPS Spectra Data are reported as a differential flux which is treated as constant over the energy range of the given spectral channel. The physical units are thus particles/cm2-sr-s-keV. The conversion from counts/s to physical unit utilize the various GFSSD given in the prior section. Currently, the assumption that we take is that the geometric factor is constant with energy; we understand the shape of the energy spectrum will affect the validity of this assumption. The instrument team routinely conducts in-flight calibration for the GFSSD values, and will release the updated values as appropriate in different mission phases. Details can be found in the calibration procedure document, EPPS_EDR2CDR.DOC, in the EPPS documentation volume. Note that this in-flight calibration is done using the science data, EPS does not have dedicated calibration files. The statistical uncertainty of the spectra data is given in the RDR. However, the current uncertainty does not include the uncertainty in the particle flux (~20% for electron, 50% for ion). The spectra are reported within 4 different classes of channels: high-resolution/low-resolution electron channels, and high-resolution/low-resolution ion channels. The channels are defined in Table 4 - Table 13. The information provided in these tables is given for each of 6 different view directions. Note that the exact boundaries given with either energies or times-of-flight are subject to change via ground commands. Table 4 - Table 13 list electron energy levels as recorded within the onboard sensors and electronics. The translations of those electronic levels to the energies of the incoming particles can be found in [6].
Table 4 EPS High and Medium Priority Spectra Ion Channels
(Based on Energy). Valid until 2007-09-06T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
0 |
80 |
|
|
1 |
80 |
82 |
|
|
2 |
82 |
87 |
|
|
3 |
87 |
103 |
|
|
4 |
103 |
156 |
|
|
5 |
156 |
330 |
|
|
6 |
330 |
897 |
|
|
7 |
897 |
2750 |
|
Table
5 EPS High
and Medium Priority Spectra Electron Channels (Based on Energy). Valid until 2007-09-06T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
0 |
29 |
|
|
1 |
29 |
30 |
|
|
2 |
30 |
32 |
|
|
3 |
32 |
37 |
|
|
4 |
37 |
57 |
|
|
5 |
57 |
120 |
|
|
6 |
120 |
326 |
|
|
7 |
326 |
1000 |
|
Table 6 EPS High and Medium Priority Spectra Ion Channels
(Based on Energy). Valid between 2007-09-06T00:00:00.000 and
2008-08-19T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
threshold |
55 |
|
|
1 |
55 |
100 |
|
|
2 |
100 |
177 |
|
|
3 |
177 |
316 |
|
|
4 |
316 |
562 |
|
|
5 |
567 |
1000 |
|
|
6 |
1000 |
1778 |
|
|
7 |
1778 |
2750 |
|
Table
7 EPS High
and Medium Priority Spectra Electron Channels (Based on Energy). Valid between 2007-09-06T00:00:00.000
and 2008-08-19T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
threshold |
20 |
|
|
1 |
20 |
36 |
|
|
2 |
36 |
65 |
|
|
3 |
65 |
115 |
|
|
4 |
115 |
204 |
|
|
5 |
204 |
244 |
|
|
6 |
244 |
434 |
|
|
7 |
434 |
1000 |
|
Table
8 EPS
High-resolution Ion Channels (Based on Energy). Valid after 2008-08-19T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
threshold |
17 |
|
|
1 |
17 |
20 |
|
|
2 |
20 |
23 |
|
|
3 |
23 |
27 |
|
|
4 |
27 |
31 |
|
|
5 |
31 |
36 |
|
|
6 |
36 |
42 |
|
|
7 |
42 |
49 |
|
|
8 |
49 |
57 |
|
|
9 |
57 |
66 |
|
|
10 |
66 |
77 |
|
|
11 |
77 |
89 |
|
|
12 |
89 |
104 |
|
|
13 |
104 |
120 |
|
|
14 |
120 |
140 |
|
|
15 |
140 |
162 |
|
|
16 |
162 |
188 |
|
|
17 |
188 |
219 |
|
|
18 |
219 |
254 |
|
|
19 |
254 |
295 |
|
|
20 |
295 |
343 |
|
|
21 |
343 |
398 |
|
|
22 |
398 |
462 |
|
|
23 |
462 |
537 |
|
|
24 |
537 |
624 |
|
|
25 |
624 |
724 |
|
|
26 |
724 |
841 |
|
|
27 |
841 |
977 |
|
|
28 |
977 |
1135 |
|
|
29 |
1135 |
1318 |
|
|
30 |
1318 |
1531 |
|
|
31 |
1531 |
1778 |
|
|
32 |
1778 |
2065 |
|
|
33 |
2065 |
2399 |
|
|
34 |
2399 |
2750 |
|
|
35 |
2750 |
5000 |
Overflow |
Table
9 EPS
High-resolution Electron Channels (Based on Energy). Valid after 2008-08-19T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
threshold |
18 |
|
|
1 |
18 |
20 |
|
|
2 |
20 |
25 |
|
|
3 |
25 |
28 |
|
|
4 |
28 |
32 |
|
|
5 |
32 |
35 |
|
|
6 |
35 |
40 |
|
|
7 |
40 |
45 |
|
|
8 |
45 |
50 |
|
|
9 |
50 |
56 |
|
|
10 |
56 |
63 |
|
|
11 |
63 |
71 |
|
|
12 |
71 |
79 |
|
|
13 |
79 |
89 |
|
|
14 |
89 |
100 |
|
|
15 |
100 |
112 |
|
|
16 |
112 |
126 |
|
|
17 |
126 |
141 |
|
|
18 |
141 |
158 |
|
|
19 |
158 |
178 |
|
|
20 |
178 |
200 |
|
|
21 |
200 |
224 |
|
|
22 |
224 |
251 |
|
|
23 |
251 |
282 |
|
|
24 |
282 |
316 |
|
|
25 |
316 |
355 |
|
|
26 |
355 |
398 |
|
|
27 |
398 |
447 |
|
|
28 |
447 |
501 |
|
|
29 |
501 |
562 |
|
|
30 |
562 |
631 |
|
|
31 |
631 |
708 |
|
|
32 |
708 |
794 |
|
|
33 |
794 |
891 |
|
|
34 |
891 |
1000 |
|
|
35 |
1000 |
5000 |
Overflow |
Table
10 EPS Low-resolution
and Summary Spectra Ion Channels (Based on Energy). Valid after 2008-08-19T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
threshold |
20 |
|
|
1 |
20 |
27 |
|
|
2 |
27 |
36 |
|
|
3 |
36 |
57 |
|
|
4 |
57 |
89 |
|
|
5 |
89 |
140 |
|
|
6 |
140 |
343 |
|
|
7 |
343 |
537 |
|
|
8 |
537 |
841 |
|
|
9 |
841 |
2065 |
|
|
10 |
2065 |
2750 |
|
|
11 |
2750 |
5000 |
Overflow |
Table
11 EPS Low-resolution
and Summary Spectra Electron Channels (Based on Energy). Valid after 2008-08-19T00:00:00.000.
|
Channel |
E1 (keV) |
E2 (keV) |
Comments |
|
0 |
threshold |
20 |
|
|
1 |
20 |
28 |
|
|
2 |
28 |
35 |
|
|
3 |
35 |
56 |
|
|
4 |
56 |
71 |
|
|
5 |
71 |
112 |
|
|
6 |
112 |
141 |
|
|
7 |
141 |
224 |
|
|
8 |
224 |
447 |
|
|
9 |
447 |
708 |
|
|
10 |
708 |
1000 |
|
|
11 |
1000 |
5000 |
Overflow |
Table
12 EPS Scan
Thresholds (keV) Fast Counts
|
Detector |
Offset A
Threshold |
Offset B
Threshold |
Offset C
Threshold |
Offset D
Threshold |
|
0 |
1.221 |
2.442 |
3.663 |
4.884 |
|
1 |
-1.221 |
0 |
1.221 |
2.442 |
|
2 |
1.221 |
2.442 |
3.663 |
4.884 |
|
3 |
-1.221 |
0 |
1.221 |
2.442 |
|
4 |
1.221 |
2.442 |
3.663 |
4.884 |
|
5 |
-1.221 |
0 |
1.221 |
2.442 |
|
6 |
42.735 |
43.956 |
45.177 |
46.398 |
|
7 |
1.221 |
2.442 |
3.663 |
4.884 |
|
8 |
42.735 |
43.956 |
45.177 |
46.398 |
|
9 |
1.221 |
2.442 |
3.663 |
4.884 |
|
10 |
42.735 |
43.956 |
45.177 |
46.398 |
|
11 |
1.221 |
2.442 |
3.663 |
4.884 |
Table
13 EPS Scan
Thresholds (keV) Shaped Counts
|
Detector |
Offset A
Threshold |
Offset B
Threshold |
Offset C
Threshold |
Offset D
Threshold |
|
0 |
-0.977 |
0.977 |
2.93 |
4.884 |
|
1 |
-1.221 |
0 |
1.221 |
2.442 |
|
2 |
-0.977 |
0.977 |
2.93 |
4.884 |
|
3 |
-1.221 |
0 |
1.221 |
2.442 |
|
4 |
-0.977 |
0.977 |
2.93 |
4.884 |
|
5 |
-1.221 |
0 |
1.221 |
2.442 |
|
6 |
40.537 |
42.491 |
44.444 |
46.398 |
|
7 |
1.221 |
2.442 |
3.663 |
4.884 |
|
8 |
40.537 |
42.491 |
44.444 |
46.398 |
|
9 |
1.221 |
2.442 |
3.663 |
4.884 |
|
10 |
40.537 |
42.491 |
44.444 |
46.398 |
|
11 |
1.221 |
2.442 |
3.663 |
4.884 |
The element that is not represented in Table 4 - Table 13 is directionality. The nominal total field-of-view (FOV) of EPS is 160° x 12°. Because the electron and ion SSDs are side-by-side, the total electron or high energy ion FOV in the long dimension is about 1/12 smaller (~13° smaller) or about 147°. And, the centers of the ion and electron FOV’s are shifted with respect to each other by ~13°. Let us define two angles within the MESSENGER spacecraft coordinate system: “alpha” is the angle from the +Y(s/c) axis and within the Y(s/c)-Z(s/c) plane (with “plus” angles viewing towards the +Z(s/c) axis); “beta” is the angle for rotations away from the Y(s/c)-Z(s/c) plane. With these definitions, the total FOV of EPS is roughly: (-80° < alpha < +80°) and (-6° < beta < +6°). The ion FOV is (-67° < alpha < +80°) and (-6° < beta < +6°). The electron FOV is (-80° < alpha < +67°) and (-6° < beta < +6°). For low energy ions (where the directionality is determined by microchannel plate anodes and not solid state detectors), the field-of-view is : (-80° < alpha < +80°) and (-6° < beta < +6°).
The direction within the ~160 degree field of view is determined for high-energy ions and for electrons with the determination of which SSD was active. With the high-energy ion and electron segments, there are a total of 12 SSD elements active at any one time. The numbering scheme for these detector elements ranges between 0 and 11, with the even SSD elements corresponding to electrons and the odd SSD elements corresponding to ions. The “0” detector (an electron detector) is the one that looks most closely aligned with the –Z(s/c) axis, while the “11” detector looks most closely to the +Z(s/c) axis. In the data that is telemetered to the ground, the directionality of the electrons and ions is represented with a number between 0 and 5. For electrons the directions (0, 1, 2, 3, 4, 5) correspond to SSDs (0, 2, 4, 6, 8, 10). For high-energy ions the directions (0, 1, 2, 3, 4, 5) correspond to SSDs (1, 3, 5, 7, 9, 11).
There is a confusing element in the representation of the directionality of low energy ions (time-of-flight only). The directionality is now determined not with the SSDs but with the microchannel plate anodes. The numbering of the TOF Start-Anodes ranges between 0 and 5. An ion or electron that passes right over Start-Anode “0” (only the ion “stimulates” this start anode) strikes either SSD 10 or SSD 11. Thus, the Start-Anodes 5, 4, 3, 2, 1, and 0 map to SSD’s (0, 1), (2, 3), (4, 5), (6, 7), (8, 9), and (10, 11), respectively. The confusing element is that the Low Energy Ion direction “5” (representing the firing of anode “5”) corresponds roughly (not exactly) to the High Energy Ion direction “0”, and the Low Energy Ion direction “0” corresponds to the High Energy Ion direction “5”. This confusing element exists for historical reasons, and because this representation is how the directionalities are indicated on board the instrument, we believed that even more confusion would be introduced if we made a change within the data generated on the ground.
In FSW6, the high-resolution spectral EDR products are integrated for T*N1 seconds, where both T and N1 are commandable parameters. They are sent to the spacecraft as a high priority packet. The low-resolution spectral EDR products contain low energy-resolution spectra as well as rate data. These packets are integrated for T and T*N1 seconds. The high-time resolution (T) packets are sent as a medium priority data product, while the lower time-resolution (T*N1) packets are called Summary Packet and are sent as high priority data, The Summary packet serves as redundant data and also provides a quick-look capability, they can be enabled or disabled by command.
New in the FSW6 is the Scan data. In scan mode, EPS varies the electronic energy thresholds (discriminators) integrating hardware rates (Fast and Shaped) at each threshold setting (defined in Table 4 - Table 13). Each of the six electronics signal processing chains consists of an Amptek charge amplifier followed by a DC-coupled unipolar shaping amplifier. The shaping time is 2.4 µs. Each shaping chain has a dedicated high-speed ADC. A settable discriminator detects the output level of the first stage of a shaping chain, which is the pole-zero compensation stage. This discriminator is called the “Fast” discriminator because the rise time of the first stage pulse is very fast and occurs within 30 ns of the particle entering the SSD. Another settable discriminator is called the “shaped” discriminator because it senses the level of the Gaussian-shaped energy pulse. The thresholds are changed three times, then the base thresholds are restored in each scan. A scan is defined as four threshold settings: three offsets and one nominal. At each threshold step, a subset of the hardware rate counters are accumulated for ¼ second. The Scan mode gives EPS the ability to lower its electronics threshold by temporary suspending the processor operation.
In addition to the rates described above, we also include particle detection error counting rates (e.g. PILEUP_E_DISCARD_RATE, REJECTED_E_RATE), which are described more fully in the EPPS EDR SIS document.
It is worth explaining here some unexpected features of the data:
- As described above, the Time of Flight segment of the instrument is no longer operational. Since early observations were made in a mode where a particle “detection” required a time of flight signal, rates and fluxes for all ION and Electron channels are all zero in the early files. Only FAST and SHAPED rates are nonzero. In later (but still pre-FSW6) measurements, the instrument was run in diagnostic mode so energy channel rates are available. The FSW6 upload allowed for an even more effective usage of the surviving (SSD) detectors.
- As of this writing, the instrument team is still developing techniques for analyzing the SCAN data. The “Delta” values in SCAN mode data are often negative. "Delta" values are an attempt to generate bounded passband-like data, but since this involves subtracting successive measurement intervals from each other, low count rate statistics frequently produce negative values.
PHA events are stored by the EPPS flight software in either the EPS High, Medium, or Low priority Science packet, for data prior to FSW6. The following explains how PHA event data are collected for data prior to the FSW6 upload on 8/18/2008. PHA events are distributed among the packet buffers in round-robin fashion: the first detected event is stored into the high-priority packet buffer, the next event is stored in the medium-priority packet buffer, and the last event is stored into the low-priority packet buffer. Please note that there is no individual time tag per PHA event.
Each event allocated to a particular buffer is simply stored into the next slot within the buffer until the buffer fills up. Thereafter, a rotating priority PHA replacement scheme is used in deciding which events may be displaced from the filled buffer. The maximum number of PHA events saved per integration period for a particular packet is shown in the following table:
Table 14 Maximum PHA Events Saved
|
EPS Packet Type |
Maximum number of PHA events saved during each accumulation interval |
|
High Priority |
10 |
|
Medium Priority |
20 |
|
Low Priority |
300 |
Note that a given EPS science packet (which may or may not contain PHA events) is time tagged with one MET (mission elapsed time) (not per PHA event). PHA events are accumulated within an integration period depending on the priority of the given science packet. Each PHA event is time tagged with the same MET associated with the science packet in which it was contained. Thus, there will be a maximum of 10 High Priority events with the same MET, 20 Medium Priority events with the same MET or 300 Low Priority events with the same MET. A given PHA CDR data file will contain the observations obtained on the same earth day and arranged in time order. Therefore a given PHA CDR data file will contain a set of N PHA events with the same MET, followed by another set of PHA events with the same MET, etc.
The FSW6 upload created a PHA packet for the express purpose of downloading PHA events. The EPS collects data for T*N1 seconds (where T=integration time and N1 is the integration time multiplier). If the integration is aborted then N1 will be the actual value instead of the commanded value. Over the T*N1 integration time, EPS saves PHA data in the order that it is seen. Each PHA packet can record a maximum of 934 PHA events. The events in a single PHA packet are time tagged with one MET time.
FSW6 also retired the high, medium, and low priority packets and consequently the capture of PHA events within those packets. The only packet which contains EPS PHA events is the EPS PHA packet and is sent down as a medium priority packet; the file naming convention will reflect that FSW6 PHA CDRs are no longer associated with a priority level.
Certain PHA events are excluded by default in standard instrument team analysis as they are of indeterminate analytical value:
- Events for which the multi-hit flag is set. (See EDR-SIS for more info).
- Events with a negative RAW Energy. For these events, the measured peak energy is less than the measured baseline energy. Presumably something (e.g. scattering off internal structures of the detector or some other non-ideal characteristic of the instrument system) has caused an incorrect measurement of the particle energy.
- Events with Maximum (= 4095) RAW Energy. This usually indicates something has gone wrong with the detection as well.
The FIPS portion of the data archive consists of five CDR data products and two ancillary calibration products. These products generally map directly from EDR data products. However, the original digital units are changed into physical units and specifics of the measurement process are removed as feasible. Additional information is also provided for some products, to facilitate science analysis. This provides the most general version of FIPS data products during the entire MESSENGER mission. Each FIPS CDR data product consists of two files. The first file contains the data in ASCII table fixed format. The second file is a detached PDS label file, which describes the contents of the ASCII table file. The label file defines the start and end time of the observation, product creation time, the structure of the ASCII table and each of the columns within the table. In addition, ancillary data products are needed to fully interpret the CDR products, an energy per charge (E/q) stepping table and a pixel field of view table, described in section 5.2.2.4. There is also a PDS label file for the E/q table file.
At the root of FIPS data are the PHA (pulse-height analyzed) word, the full-capability measurements of single particle events. For each event, FIPS measures the TOF, E/q and location on the start MCP in the form of Wedge, Strip and Zigzag values from the position-sensing anode. The FIPS hardware also classifies the event as proton or heavy ion via an uploaded TOF threshold, different for each E/q step. Because it is not always possible to telemeter all of these PHA words to the ground, other data products are built up from the PHA words. This gives rise to three types of data products upon which FIPS CDR data are based:
Table
15 FIPS Data
|
Type |
Description |
|
Pulse Height Analyzed (PHA) event words |
Individual ion event measurements of E/q, TOF and MCP location, along with additional information to allow nearly self-contained data analysis. PHA quantities are given in digital and physical units. Digital units are retained to simplify some data analysis, e.g. digital units provide natural binning for histograms. Time-of-flight is given in channels and nanoseconds. Energy per charge is given in deflection voltage step and keV/e. MCP location is given digital X-Y MCP position and incident zenith and azimuthal angles (degrees).
Additional quantities to facilitate self-contained analysis are m/q (amu/e), type (binary, proton (1) or heavy (0)), weight (unitless). The weight represents a combination of instrument-related factors such as efficiency and angle dependence. |
|
Differential intensity spectra |
Differential intensity spectra are 1-D histograms of event differential intensity at each E/q step, integrated over incident angle. Differential intensity spectra are given in units of counts (keV/e)-1 sec-1 cm-2. |
|
Velocity Distributions |
Velocity distributions are 2-D histograms of event probability at each MCP X-Y location (incident solid angle), summed over E/q step. Normalized velocity distributions are given as unit-less probabilities. A value at a particular X-Y location is the probability of events at that location. Three specific velocity distribution function types are provided as available from the FIPS data stream: 1) heavy ions (8x8) 2) proton (8x8) 3) high resolution proton (32x32). |
To allow the PHA event data to function as a nearly stand-alone data product, several additional quantities are included in CDR PHA data.
Using a relation derived from calibration data, these MCP X-Y positions are mapped to incident zenith and azimuthal angles. The zenith angle is measured from the FIPS boresight vector (z axis in FIPS Cartesian), the cylindrical symmetry axis of FIPS electrostatic analyzer and given as an angle between 15 and 70 degrees. The azimuthal angle records the angle around this symmetry axis, beginning at the y axis in the FIPS Cartesian coordinate system, as defined in the MESSENGER SPICE Frames Kernel. After conversion to the FIPS Cartesian coordinate system, these angles can be transformed to other coordinate systems by using SPICE. The combination of spacecraft body and heat shield effectively block FIPS field-of-view (FOV) through approximately zenith angles [25,75] and azimuthal angles [270,10] (70 degrees). The solar array on the –X side of the spacecraft, also blocks FIPS FOV to a small and variable degree. Exact locations of blockages, as a function of time, can be extracted from the EPPS-specific SPICE kernel.
To facilitate ion identification,
mass per charge (M/q, in AMU/e, where AMU is Atomic Mass Unit) for each PHA
word is calculated as a function of E/q step and TOF, according to the
following equation:
M/q = 2 (k * U + |Va| - UL
) * TOF 2 / ( d2 * 1040 ns2
keV / cm2 amu)
where:
k
= deflection system constant, approx 1.33
U=
deflection system voltage, in kV
Va=
post acceleration voltage, in kV
UL
= energy lost to carbon foil
TOF
= the measured Time-of-flight, in ns
d
= distance over which TOF is measured, in cm.
This equation includes only
rudimentary effects of carbon foil energy loss and scattering. These tend to spread the calculated M/q
values for each species. As data are
analyzed throughout the mission, the contribution of these effects will be
revised to reflect increased understanding of FIPS performance.
The weighting factor represents the weight that each PHA word should be given in analysis, and includes effects from several instrument performance parameters, such as energy and angle-dependent efficiencies. The detailed explanation of this parameter is beyond the scope of this document.
For a subset
of these events, the flight software (FSW) performs calculations to reduce the
number of bits required for each PHA word, from 53 bits to 28 bits. The least significant bit (LSB) of the TOF
value is dropped, 11 to 10 bits. The
three 12 bit Wedge (w), Strip (s), and Zigzag (z) values are converted to two 6
bit X and Y positions, using the calculations below (offsets are set by ground
command):
w = w – wedge_offset
s = s – strip_offset
z = 14*(z – zigzag_offset)/10
sum = w + s + z
X = 128*(w + (w-z)/5)/sum
Y = 128*(s + (s-z)/5)/sum
There are
slight changes to these equations for FSW7, which are detailed below.
To provide high-level view of ion
events, FIPS CDR data includes five one-dimensional differential intensity
spectra, each with 64 elements (Table 16). The first four differential
intensities are based on counters retrieved from FIPS hardware while the fifth
differential intensity, Events Processed, is based on a software counter. Each of these is recorded at every E/q step
to provide an E/q spectrum. Since the
instrument can run in several modes with different E/q stepping sequences, care
must be taken to match the proper sequence to the data. These inherently 24 bit rate counters are
compressed using a 10 bit logarithmic compression code, 5 bits for mantissa and
5 bits for exponent (5/5 compression). While the rate counters have been
decompressed as part of the conversion to CDR data, there is a loss in accuracy
that remains from the compression. In
most contexts these losses are very small and can be ignored in science
analysis.
Table 16 Differential Intensity Spectra
|
Data
Item |
Description |
|
Start Differential intensity |
Differential intensity of events which
trigger a signal on the start MCP |
|
Stop Differential intensity |
Differential intensity of events which trigger a signal on
the stop MCP |
|
Valid Event Differential intensity |
Differential intensity of events which trigger both a
start and stop signal. |
|
Proton Differential intensity |
Differential intensity of valid events which are
classified as protons by falling under TOF threshold for the E/q step in
which they are collected. |
|
Events Processed Differential intensity |
Differential intensity of events which are processed by
the FSW. |
The Start and Stop differential
intensities are not particularly suitable for science analysis. The Valid Event and Proton differential
intensities provide a convenient overview of the data (per E/q step) when
angular and TOF information is not needed.
The heavy ion differential intensity can be derived by taking the
difference of these two differential intensities, Valid Event –
Proton. The Events Processed
differential intensity can be used to show the fraction of events that have
been registered in hardware but not processed in software (due to time
limitations) by simply dividing Events Processed differential intensity by
Valid Event differential intensity.
FIPS is an imaging instrument that
views into a region of solid angle that has conical symmetry and is
bounded by 2 nested cones, with half angles of ~15
and ~75 degrees. The field of view
symmetry axis points in the direction of the following unit vector, (-0.74324,
-0.383558, 0.548158), in spacecraft coordinates. Inside the TOF region of FIPS, this field of
view is mapped onto a Cartesian X-Y coordinate system on the Start MCP, with
binned elements up to a resolution of 64 x 64.
Distributions of the X-Y positions for each PHA represent the
distributions of the velocity directions of particle events and are stored as
2D arrays of probabilities in CDR data.
Furthermore, the value at a given X-Y position represents the fraction
of total proton events which fell in that X-Y bin for the scan in
question. An estimate of the
differential flux for this X-Y bin can be calculated by the product of this
probability with the sum of the proton differential flux spectrum for the
scan. The resolution of these 2D arrays
with respect to the X-Y MCP coordinate system is described below. FIPS produced velocity distributions for
protons and heavy ions (via selected M/q ranges) at a variety of angular
resolutions. However, only the
normalized proton velocity distributions are included in CDR data. Flyby data analysis showed that all heavy ion
PHAs were transmitted to the ground with considerable margin. As such, heavy ion velocity distributions,
produced at low angular resolution, were found to be inferior to distributions
constructed on the ground.
Due to changes in FSW and downlink capabilities, FIPS data products have changed over the course of the mission. These changes, while greatly improving quality of the data, make the mapping of data types into particular CDR data products (i.e. files) a little more complicated. Specific FIPS data products at the CDR level are listed in Table 17.
Data products are time-tagged at the end of the accumulation interval. A given PHA CDR data file contains observations made on the same earth day and arranged in time order.
Table
17 FIPS
CDR Data Products
|
Product |
Description |
|
PHA Event Words |
Events collected in scans 1-10 of the 10 scan sequence. Sequence and Scan PHA words are 28 bit, while Raw PHA words are the full 53 bits. Maximum number of PHA words which can be stored per scan depends on source packet. Sequence, Scan and Raw packets can store 64, 128 and 617 PHA words, resp. See EPPS EDR SIS for packet details. This information is not required for most science data analysis. PHA words are time-tagged for the scan in which they were measured, so multiple PHA words have the same time tag. |
|
High Priority Spectra |
Differential intensity spectra collected in scan 10 of the 10 scan sequence. Normalized proton velocity distribution (8x8) for scan 10 of the 10 scan sequence. These products were retired after July 7, 2009. Flight Software changes obviated the need for their continued production. |
|
Medium Priority Spectra |
Differential intensity spectra collected in scans 1-9 of the 10 scan sequence. Normalized proton velocity distribution (8x8) for scans 1-9 of the 10 scan sequence. These products were retired after August 18, 2008. Flight Software changes obviated the need for their continued production. |
|
Scan Spectra |
Differential intensity spectra collected in scans 1-9 of the 10 scan sequence. |
|
High Resolution Normalized Proton Velocity Distributions |
High resolution normalized proton velocity distribution (32x32) for scans 1-10 of the 10 scan sequence. These products were retired after July 7, 2009. Flight Software changes obviated the need for their continued production. |
Energy per charge stepping tables (FIPA_E*) and pixel field of view (FIPA_F*) tables are included as an ancillary data product in the CALIBRATION directory of the archive document volume. The Energy per charge stepping files contain the E/q value in keV/e as a function of E/q step number for each of the 8 stepping tables loaded into the instrument. The stepping table used at a particular time is given by the FIPS_SCANTYPE variable in the CDR data. The Pixel Field of View files contain lists of the pixels in the FIPS FOV.
Data quality is assessed in a very simple manner: If FIPS was on in a nominal configuration, the data are marked as good. To minimize the amount of data affected, data quality is reported on a record by record basis.
As flight data was returned from FIPS, bugs in data processing were discovered and areas for improvement of data products identified. The largest motivation for change was the substantial increase in allowed data volume. This came as the mission operations team increased downlink rates and reduced margins from pre-launch predictions, as knowledge of actual system throughput was gained from actual usage in space. The following table summarizes the impacts of these changes on CDR data.
Table 18 Impact of FSW Changes on CDR Data
|
FSW |
Upload Date |
Impact of change on CDR data |
|
FSW41 |
(pre-launch) |
n/a |
|
FSW5 |
06 Sep 2007 |
Fixed bugs in PHA X-Y calculation which caused overflow values to be mapped into valid range. Added PHA buffer to provide even distribution of PHA words across E/q step. Added Stop differential intensity for every step of every scan. |
|
FSW6 |
18 Aug 2008 |
Added high-resolution normalized proton velocity distributions (32x32) because flyby data showed that 8x8 resolution was insufficient. PHA X-Y calculation changed to maximize coverage this data product. |
|
FSW7 |
18 Aug 2009 |
Simplified data processing to PHAs and differential intensity spectra only. Proton events now included as 28 bit PHA event words and decimated according to commanded limits. Heavy ions only transmitted as 53 bit PHA event words and no longer buffered. Velocity distributions eliminated. |
Notes: 1)
Collection of flight data starts with FSW version 4. FSW versions 1-3 were used only in
development and ground testing.
Prioritization of PHA words for
downlink was done in a very simple fashion in FSW v4. Two PHA word slots were allocated per E/q
step. Slots left unfilled were available
for PHAs from subsequent steps. The
effect of this scheme was to bias PHA collection toward higher E/q steps, which
occur first in the sequence. With FSWv5, a buffered, rotating priority scheme
was added which allowed a more even distribution of PHAs in E/q, while
maximizing the number of PHA words transmitted within the telemetry limit. As events are collected, the flight software
stores up to 12 events per deflection system voltage step in a buffer. At the end of the scan, these events are read
out in voltage step order, one from each voltage step. Within a voltage step, PHAs are read out in
the same order that they were stored.
When no PHA exists for a given voltage step, one is read from the next
voltage step which has PHAs remaining, until the allowed number of PHAs (quota
as provided in Table 17) for this scan have been selected.
In FSW7, the buffering scheme was removed entirely and no per-E/q step
limits imposed on the number of PHA words.
This change was justified by results of modeling, based on heavy ion
count rate profiles from flyby data.
This modeling showed that all heavy ion PHA words could be transmitted
to the ground with considerable margin, making the buffer unnecessary. Since the buffer decreased processing
throughput and was deemed unnecessary, it was removed.
As of FSW7, proton events are included in telemetry as 28 bit PHA words. To limit proton data volume, the FIPS hardware can decimate the proton events, i.e. send only a fraction of those collected, 1 in 2n, where n is the decimation level. The flight software controls the decimation level, incrementing it when scan or orbit based limits are exceeded. This decimation level is included in CDR data.
Velocity distributions in FSW
versions 4 & 5 are very coarse, with the natural 64x64 X-Y coordinates
binned into 8x8 arrays. For a particular
X-Y pair, the row and column of the bin in which to increment are given by X/8
and Y/8. In
FSW v6, a much higher resolution normalized proton velocity distribution of
32x32 bins was added. For this version,
the values X/2 and Y/2 are used as the row and column within
the velocity distribution matrix to give the bin to
be incremented. A slightly different
Wedge, Strip, Zigzag to X-Y calculation was used to maximize coverage in these
32x32 normalized proton velocity distribution, detailed in Table 19.
Table 19 Equations for X, Y
|
FSW4, FSW5, & FSW7 |
FSW6 |
|
X = 128*(w + (w-z)/5)/sum |
X = 96*(s + (s-z)/5)/sum |
|
Y = 128*(s
+ (s-z)/5)/sum |
Y = 100*(s + 2*(s-z)/11)/sum |
There will be one EPPS PDS Documentation Archive Volume and one EPPS PDS Data Archive Volume. The data volume will contain level 3 CODMAC (Committee on Data Management and Computation) data products, also known as CDRs. Each product will have a unique file name and conform to the file naming convention in section 6.5. All CDR products will be stored at the Applied Physics Laboratory/Science Operations Center (APL/SOC) during mission operations. Volumes will be electronically transferred to the PDS PPI Node following the procedure in section 5.3.3.
The EPPS CDR files will be produced by the MESSENGER Science Operations Center (SOC) using data processing routines provided by the EPS and FIPS teams. A Java program derived from the MIDL (Mission Independent Data Layer) analysis software developed by APL is used to convert the EPS EDR data to CDRs. The FIPS data are produced using three software routines, written in the IDL programming language: mfips_decode_pha.pro, mfips_decode_rates.pro and mfips_decode_hrpvd.pro. The CDR data products are made available to the MESSENGER Science Team for initial evaluation and validation. At the end of the evaluation and validation period, the data are organized and stored in the directory structure described in section 6.8 for transmittal to the PPI Node. The transmittal process is described in the following section, Data Flow. An initial release of the documentation volume will accompany the initial release of the data volume. Thereafter, there will be updates to the documentation volume whenever the EPPS team determines that they have a sufficiently improved calibration to warrant a new release. PDS will then provide public access to the data products through its online distribution system. These products will be used for engineering support, direct science analysis, and construction of other science products.
The
MESSENGER SOC operates under the auspices of the MESSENGER Project Scientist to
plan data acquisition, generate, and validate data archives. The SOC supports
and works with the MOC, the Science Team, instrument scientists, and the PDS.
Figure 2 MESSENGER Data Flow shows the flow of data within the MESSENGER project and out to PDS. The MOC handles raw data flow to and from the MESSENGER spacecraft and the SOC converts the raw telemetry into EDRs, which are subsequently converted into CDRs. The Science Team validates the CDRs and implements corrections if needed. Documentation and CDRs are delivered to the PDS Planetary Plasma Interactions (PPI) node. All SPICE kernels used in CDR processing are delivered to the PDS Navigation and Ancillary Information (NAIF) node. The delivery process is detailed below.
Figure 1 MESSENGER data flow
The MESSENGER SOC will deliver data for the EPPS CDR data volume to the PDS PPI
Node in standard product packages. Each package will comprise data and
ancillary data files, organized into directory structures consistent with the
volume design described in section 6.8.
The initial release will also contain the documents and required files for the
EPPS documentation volume, organized into directory structures as described in
section 6.7.
Subsequent releases to the EPPS documentation volume will be at the discretion
of the EPPS team and be delivered whenever the EPPS team determines that they
have a sufficiently improved calibration to warrant a new release.
The following describes the electronic transfer process of releasing data to PDS for both the data volume and the documentation volume. This process will be implemented for the first PDS delivery. Future data deliveries will be assumed to follow the same process unless otherwise noted in an update of this document. Given the long duration of the mission the project reserves the option of exploring alternate data delivery methods for subsequent deliveries. As such, the method of electronic transfer may change and will be revised accordingly in the SIS. Any changes to the delivery process will be noted in an update to the SIS document and will include the specific dates which will use the new delivery process. The delivery of products to the data volume will follow the schedule in [2]. The delivery date for updates to the documentation volume will be determined as needed at the discretion of the EPPS team.
In the week prior to the delivery date the directory structure will be compressed into a single “zip archive” file for transmittal to the PDS node. The zip archive preserves the directory structure internally so that it can be recreated after electronic delivery to the PDS node. The zip archive file is transmitted to the PDS node via FTP (file transfer protocol) to an account set up by the receiving node. Also transmitted will be a checksum file created using the MD5 algorithm. This provides an independent method of verifying the integrity of the zip file after it has been sent. Within days of transmittal the PDS node will acknowledge receipt of the archive and checksum file. If acknowledgement is not received, or if problems are reported, the MESSENGER SOC will immediately take corrective action to effect successful transmittal.
After transmittal the PDS node will uncompress the zip archive file and check for data integrity using the checksum file. The node will then perform any additional verification and validation of the data provided and will report any discrepancies or problems to the MESSENGER SOC. It is expected that the node will perform these checks in about two weeks. After inspection has been completed to the satisfaction of the PDS node, the node will issue to the MESSENGER SOC acknowledgement of successful receipt of the data.
Following receipt of a data delivery the PDS node will organize the data into a PDS volume archive structure within its online data system. Newly delivered data will be made available publicly from PDS once accompanying labels and other documentation have been validated.
The PDS label conforms to PDS version
3.8 standards. For more information about this
standard consult the PDS Standards Reference Document. The label is detached
and in a separate PDS label file. The purpose of the PDS label is to describe
the data product and provide ancillary information about the data product.
There is a PDS label file for every EPPS CDR data file. There is one
DATA_SET_ID assigned to the EPPS CDR data. The CDRs are further grouped into
data products and are identified by the STANDARD_DATA_PRODUCT_ID keyword and
the file naming convention, section 6.5. Example label file content is
shown here for every CDR data product. Note that the data are contained within
an ASCII table and the details of the table structure are described by an
external ASCII format file (*.FMT). The Columns in each format file are
described separately in the Appendix.
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
940
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
21680
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSH_S2008014CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:22:32
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_HI_SPEC_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"MERCURY 1 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-014T00:01:41.123
STOP_TIME = 2008-014T23:59:27.081
^HEADER =
("EPSH_S2008014CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSH_S2008014CDR_V1.TAB", 4)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 3
BYTES = 65040
DESCRIPTION = "The first 3 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 114
INTERCHANGE_FORMAT =
ASCII
ROWS = 940
ROW_BYTES = 21680
DESCRIPTION = "
This table contains spectral data collected
by the MESSENGER EPS
instrument in High Priority Mode.
The complete column definitions are
contained in an external file
found in the LABEL directory of the archive
volume. Additional
details are contained in the CDR SIS
document."
NOTE =
"Data Quality: 0"
^STRUCTURE = "EPSHIGH_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
2872
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
21392
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSM_S2006059CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:24:46
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_MED_SPEC_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"VENUS 1 CRUISE"
TARGET_NAME = "CALIBRATION"
START_TIME = 2006-059T00:00:28.084
STOP_TIME = 2006-059T23:59:50.150
^HEADER = ("EPSM_S2006059CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSM_S2006059CDR_V1.TAB", 4)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 3
BYTES = 64176
DESCRIPTION = "The first 3 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 113
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 21392
ROWS = 2872
DESCRIPTION = "
This table contains spectral data collected
by the MESSENGER EPS
instrument in Medium Priority Mode.
The complete column definitions are
contained in an external file
found in the LABEL directory of the archive
volume. Additional
details are contained in the CDR SIS
document."
NOTE = "Data Quality: 0"
^STRUCTURE = "EPSMED_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The format for the EPS High, Medium, Low Priority PHA PDS Labels are identical in terms of the PDS keywords used. In addition, the format of the PHA TABLE object is the same for all EPS PHA CDRs. Therefore, only one FORMAT file is used to describe all PHA TABLE objects. The file naming convention will distinguish whether the EPS PHA CDR contains high, medium, or low priority PHA data.
After the FSW6 upload, the only packet which may contain EPS PHA events is the EPS PHA packet. There is no longer any association with high, medium or low priority as of FSW6 for EPS PHA CDRs. Section 6.5 File Naming Conventions will explain the designation for N/A priority in the filename.
A sample High Priority PDS PHA label is shown below:
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
358746
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
359
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSN_P2008014CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:24:57
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_PULSE_HEIGHT_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"MERCURY 1 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-014T00:00:09.027
STOP_TIME = 2008-014T23:59:56.168
^HEADER = ("EPSN_P2008014CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSN_P2008014CDR_V1.TAB", 3)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS
= 2
BYTES = 718
DESCRIPTION = "The first 2 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT =
HEADER
OBJECT = ASCII_TABLE
COLUMNS = 21
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 359
ROWS = 358746
DESCRIPTION = "
This table contains the Pulse Height
Analysis (PHA) data collected by
the MESSENGER EPS instrument.
The complete column definitions are
contained in an external file found
in the LABEL directory of the archive
volume. Additional details are
contained in the CDR SIS document."
NOTE = "Data Quality: 0"
^STRUCTURE = "EPS_PHA_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The High Resolution EPS Spectra CDR was created as the result of the FSW6 upload. It stores the high resolution ion and electron spectral data collected by the EPS instrument.
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
288
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
40496
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSH_R2008281CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:24:31
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_HIRES_SPEC_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"MERCURY 2 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-281T00:01:12.036
STOP_TIME = 2008-281T23:56:12.036
^HEADER = ("EPSH_R2008281CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSH_R2008281CDR_V1.TAB", 4)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 3
BYTES = 121488
DESCRIPTION = "The first 3 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 56
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 40496
ROWS = 288
DESCRIPTION = "
This table contains high-resolution spectra
data collected by
the MESSENGER EPS instrument.
The complete column definitions are
contained in an external file found
in
the LABEL directory of the archive volume. Additional details are
contained in the CDR SIS document."
NOTE = "Data Quality: 0"
^STRUCTURE = "EPS_HIRES_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The Low Resolution EPS Spectra CDR was created as the result of the FSW6 upload. It stores the low resolution ion and electron spectral data as well as rate counters collected by the EPS instrument.
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
2878
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
13640
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSL_R2008281CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:24:38
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_LORES_SPEC_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"MERCURY 2 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-281T00:00:12.036
STOP_TIME = 2008-281T23:59:42.126
^HEADER = ("EPSL_R2008281CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSL_R2008281CDR_V1.TAB", 4)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 3
BYTES =
40920
DESCRIPTION = "The first 3 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 67
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 13640
ROWS = 2878
DESCRIPTION = "
This table contains low-resolution spectra
data collected by
the MESSENGER EPS instrument.
The complete column definitions are
contained in an external file found
in the LABEL directory of the archive
volume. Additional details are
contained in the CDR SIS document."
NOTE = "Data Quality: 0"
^STRUCTURE = "EPS_LORES_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The EPS Summary Spectra CDR was created as the result of the FSW6 upload. It contains integrated rates and low resolution spectra collected by the EPS instrument.
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
288
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
13640
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSS_S2008282CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:25:22
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_SUM_SPEC_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"MERCURY 2 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-282T00:01:12.036
STOP_TIME =
2008-282T23:56:12.036
^HEADER = ("EPSS_S2008282CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSS_S2008282CDR_V1.TAB", 4)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 3
BYTES = 40920
DESCRIPTION = "The first 3 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 67
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 13640
ROWS = 288
DESCRIPTION = "
This table contains summary spectra data
collected by
the MESSENGER EPS instrument.
The complete column definitions are
contained in an external file found
in the LABEL directory of the archive
volume. Additional details are
contained in the CDR SIS document."
NOTE = "Data Quality: 0"
^STRUCTURE = "EPS_SUM_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The EPS Scan CDR was created as the result of the FSW6 upload. It contains integrated hardware rates for four energy threshold settings. Each threshold setting and integration lasts ¼ second.
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS =
70
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
14000
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "EPSS_R2008280CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:25:15
PRODUCT_TYPE =
"CDR"
STANDARD_DATA_PRODUCT_ID =
"EPS_SCAN_SPEC_CDR"
SOFTWARE_NAME =
"MIDLMessengerCDRGenerator"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME =
"ENERGETIC PARTICLE SPECTROMETER"
INSTRUMENT_ID =
"EPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-EPS-CDR-V1.0"
DATA_SET_NAME =
"MESSENGER E/V/H/SW EPPS CALIBRATED EPS CDR
V1.0"
MISSION_PHASE_NAME =
"MERCURY 2 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-280T03:35:02.006
STOP_TIME = 2008-280T14:46:11.033
^HEADER = ("EPSS_R2008280CDR_V1.TAB", 1)
^ASCII_TABLE =
("EPSS_R2008280CDR_V1.TAB", 4)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 3
BYTES = 42000
DESCRIPTION = "The first 3 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 56
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 14000
ROWS = 70
DESCRIPTION = "
This table contains scan rates collected by
the MESSENGER EPS instrument.
The complete column definitions are
contained in an external file found
in the LABEL directory of the archive
volume. Additional details are
contained in the CDR SIS document."
NOTE = "Data Quality: 0"
^STRUCTURE = "EPS_SCAN_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The
following are example label headers for the FIPS CDR products. As with the EPS
CDRs all table structures are defined by external format files. The Columns in
each format file are defined separately in the Appendix.
PDS_VERSION_ID =
"PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS = 424
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES = 4277
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPH_S2008014CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:20:59
PRODUCT_TYPE = "CDR"
STANDARD_DATA_PRODUCT_ID =
"FIPS_HI_SPECTRA_CDR"
SOFTWARE_NAME = "mfips_decode_rates.pro"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "FAST IMAGING PLASMA SPECTROMETER"
INSTRUMENT_ID = "FIPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
SOURCE_PRODUCT_ID =
{"FIPA_E2007210CDR_V1.TAB"}
MISSION_PHASE_NAME =
"MERCURY 1 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-014T00:11:21.000
STOP_TIME = 2008-014T23:59:46.000
SPACECRAFT_CLOCK_START_COUNT =
"108756862.000"
SPACECRAFT_CLOCK_STOP_COUNT =
"108842567.000"
^HEADER = ("FIPH_S2008014CDR_V1.TAB",1)
^ASCII_TABLE = ("FIPH_S2008014CDR_V1.TAB",6)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 5
BYTES =
21385
DESCRIPTION = "The first 5 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT =
ASCII_TABLE
COLUMNS = 10
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 4277
ROWS = 424
DESCRIPTION = "
This table contains the following data
gathered by the Fast Imaging
Plasma Spectrometer (FIPS) in HIGH priority
mode:
-Normalized proton velocity distribution
-Differential intensity spectra
The complete column definitions are
contained in an external file
found in the LABEL directory of the archive
volume. Energy per
charge (E/q) tables referenced in
SOURCE_PRODUCT_ID are located in
the CALIBRATION directory of the archive
volume. Additional details
are contained in the CDR SIS
document."
^STRUCTURE =
"FIPS_HI_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
A
FSW6 upload was implemented on 8/19/2008. The upload retired the Medium
Priority packet and split the contents into two new packets. As a result, the
Medium Priority CDR is no longer created after 8/18/2008. Data from the two new
packets are contained in the FIPS Scan and FIPS Hi-Res Normalized proton
velocity distribution CDRs.
PDS_VERSION_ID = "PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS = 795
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES = 4277
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPM_S2006060CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:21:12
PRODUCT_TYPE = "CDR"
STANDARD_DATA_PRODUCT_ID =
"FIPS_MED_SPEC_CDR"
SOFTWARE_NAME = "mfips_decode_rates.pro"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "FAST IMAGING PLASMA SPECTROMETER"
INSTRUMENT_ID = "FIPS"
DATA_SET_ID =
"MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
SOURCE_PRODUCT_ID =
{"FIPA_E2006057CDR_V1.TAB"}
MISSION_PHASE_NAME =
"VENUS 1 CRUISE"
TARGET_NAME = "CALIBRATION"
START_TIME = 2006-060T00:00:02.000
STOP_TIME = 2006-060T15:55:58.000
SPACECRAFT_CLOCK_START_COUNT =
"49658437.000"
SPACECRAFT_CLOCK_STOP_COUNT =
"49715793.000"
^HEADER = ("FIPM_S2006060CDR_V1.TAB", 1)
^ASCII_TABLE = ("FIPM_S2006060CDR_V1.TAB", 6)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 5
BYTES = 21385
DESCRIPTION = "The first 5 records of this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS =
10
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 4277
ROWS = 795
DESCRIPTION = "
This table contains the following data
gathered by the Fast Imaging
Plasma Spectrometer (FIPS) in MEDIUM
priority mode:
-Normalized proton velocity distribution
-Differential intensity spectra
The complete column definitions are
contained in an external file
found in the LABEL directory of the archive
volume. Energy per
charge (E/q) tables referenced in
SOURCE_PRODUCT_ID are located in
the CALIBRATION directory of the archive
volume. Additional details
are contained in the CDR SIS
document."
^STRUCTURE = "FIPS_MED_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The format for the FIPS High,
Medium, Low PHA PDS Labels are identical in terms of the PDS keywords
used. In addition, the format of the
PHA_TABLE object is the same for all FIPS PHA CDRs. Therefore, only one FORMAT
file is used to describe all PHA_TABLE objects.
After the FSW6 upload, the only
packets which may contain PHA events are the high priority, low priority, and
scan packets (medium priority packets being retired). The file naming convention
will distinguish whether the FIPS PHA CDR contains PHA events extracted from
high or low priority, or scan packets.
This is detailed in Section 6.5.
A sample PHA PDS label is shown below:
PDS_VERSION_ID = "PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS = 7956
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES = 159
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPP_P2006059CDR_V1"
PRODUCT_VERSION_ID
= "V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:21:20
PRODUCT_TYPE = "CDR"
STANDARD_DATA_PRODUCT_ID =
"FIPS_PHA_CDR"
SOFTWARE_NAME = "mfips_decode_pha.pro"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "FAST IMAGING PLASMA SPECTROMETER"
INSTRUMENT_ID = "FIPS"
DATA_SET_ID =
"MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
SOURCE_PRODUCT_ID =
{"FIPA_E2006057CDR_V1.TAB","Weight"}
MISSION_PHASE_NAME =
"VENUS 1 CRUISE"
TARGET_NAME = "CALIBRATION"
START_TIME = 2006-059T00:00:05.000
STOP_TIME = 2006-059T23:58:57.000
SPACECRAFT_CLOCK_START_COUNT =
"49572039"
SPACECRAFT_CLOCK_STOP_COUNT =
"49658372"
^HEADER = ("FIPP_P2006059CDR_V1.TAB", 1)
^ASCII_TABLE = ("FIPP_P2006059CDR_V1.TAB", 5)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 4
BYTES = 636
DESCRIPTION = "The first 4 records of this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS =
18
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 159
ROWS = 7956
DESCRIPTION = "
This table contains the Pulse Height
Analysis (PHA) data collected by
the MESSENGER Fast Imaging Plasma
Spectrometer (FIPS).
The complete column definitions are
contained in an external file
found in the LABEL directory of the archive
volume. Energy per
charge (E/q) tables referenced in
SOURCE_PRODUCT_ID are located in
the CALIBRATION directory of the archive
volume. Additional details
are contained in the CDR SIS
document."
^STRUCTURE = "FIPS_PHA_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The FIPS Scan CDR contains FIPS differential intensity spectra at each Deflection System High Voltage (DSHV) step in a scan.
PDS_VERSION_ID = "PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS = 1163
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES = 3573
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPS_R2008281CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:22:02
PRODUCT_TYPE = "CDR"
STANDARD_DATA_PRODUCT_ID =
"FIPS_SCAN_CDR"
SOFTWARE_NAME = "mfips_decode_pha.pro"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "FAST IMAGING PLASMA SPECTROMETER"
INSTRUMENT_ID = "FIPS"
DATA_SET_ID =
"MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
SOURCE_PRODUCT_ID =
{"FIPA_E2007210CDR_V1.TAB"}
MISSION_PHASE_NAME =
"MERCURY 2 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-281T00:01:33.000
STOP_TIME = 2008-282T00:00:51.000
SPACECRAFT_CLOCK_START_COUNT =
"131825074.000"
SPACECRAFT_CLOCK_STOP_COUNT =
"131911432.000"
^HEADER = ("FIPS_R2008281CDR_V1.TAB", 1)
^ASCII_TABLE = ("FIPS_R2008281CDR_V1.TAB", 6)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 5
BYTES = 17865
DESCRIPTION = "The first 5 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 9
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES =
3573
ROWS = 1163
DESCRIPTION = "
This table contains the FIPS differential
intensity spectra gathered by the Fast Imaging
Plasma Spectrometer (FIPS) accumulated over
each separate observation.
The complete column definitions are
contained in an external file
found in the LABEL directory of the archive
volume. Energy per
charge (E/q) tables referenced in
SOURCE_PRODUCT_ID are located in
the CALIBRATION directory of the archive
volume. Additional details
are contained in the CDR SIS
document."
^STRUCTURE = "FIPS_SCAN_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The FIPS HRPVD CDR contains a 32 x 32 high resolution normalized proton velocity distribution, integrated over a 10 scan sequence.
PDS_VERSION_ID = "PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS = 129
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES = 12385
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPS_V2008281CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2010-01-05T17:21:06
PRODUCT_TYPE = "CDR"
STANDARD_DATA_PRODUCT_ID =
"FIPS_HIRES_P_V_CDR"
SOFTWARE_NAME = "mfips_decode_hrpvd.pro"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "FAST IMAGING PLASMA SPECTROMETER"
INSTRUMENT_ID = "FIPS"
DATA_SET_ID =
"MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
SOURCE_PRODUCT_ID =
{"FIPA_E2007210CDR_V1.TAB"}
MISSION_PHASE_NAME =
"MERCURY 2 FLYBY"
TARGET_NAME = "MERCURY"
START_TIME = 2008-281T00:09:21.000
STOP_TIME = 2008-281T23:55:17.000
SPACECRAFT_CLOCK_START_COUNT =
"131825542.000"
SPACECRAFT_CLOCK_STOP_COUNT =
"131911098.000"
^HEADER = ("FIPS_V2008281CDR_V1.TAB", 1)
^ASCII_TABLE = ("FIPS_V2008281CDR_V1.TAB", 6)
OBJECT =
HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 5
BYTES = 61925
DESCRIPTION = "The first 5 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 40
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES = 12385
ROWS = 129
DESCRIPTION = "
This table contains the high-resolution
normalized proton velocity distributions
gathered by the Fast Imaging Plasma
Spectrometer (FIPS)collected over
a 10-scan sequence. The complete column
definitions are contained in
an external file found in the LABEL
directory of the archive volume.
Energy per charge (E/q) tables referenced
in SOURCE_PRODUCT_ID are
located in the CALIBRATION directory of the
archive volume. Additional
details are contained in the CDR SIS
document."
^STRUCTURE = "FIPS_HRPVD_CDR.FMT"
END_OBJECT = ASCII_TABLE
END
The FIPS EQ ancillary data contains the energy per charge tables.
PDS_VERSION_ID = "PDS3"
/*
** FILE FORMAT ** */
FILE_RECORDS = 69
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES =
264
/*
** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPA_E2004216CDR_V1"
PRODUCT_VERSION_ID =
"V1"
PRODUCT_CREATION_TIME =
2009-07-14T22:01:30
PRODUCT_TYPE = "ANCILLARY_DATA"
STANDARD_DATA_PRODUCT_ID =
"FIPS_E_PER_CHARGE"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "FAST IMAGING PLASMA SPECTROMETER"
INSTRUMENT_ID = "FIPS"
DATA_SET_ID = "MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
^HEADER = ("FIPA_E2004216CDR_V1.TAB",5)
^TABLE = ("FIPA_E2004216CDR_V1.TAB",6)
OBJECT =
HEADER
^HEADER_TYPE =
TEXT
INTERCHANGE_FORMAT =
"ASCII"
RECORDS = 5
BYTES = 1320
DESCRIPTION = "The first 5 records of
this
file are the header section. The header
contains column
headings to improve usability."
END_OBJECT = HEADER
OBJECT = TABLE
COLUMNS = 33
INTERCHANGE_FORMAT =
ASCII
ROW_BYTES
= 264
ROWS = 64
DESCRIPTION = "
This table contains the E/q value (keV/e),
accumulation time (ms) and
proton threshold (ns) as a function of E/q
step number, for each of the
8 stepping tables loaded into the
instrument. The stepping table used
at a particular time is given by the
FIPS_SCANTYPE variable in the FIPS
CDR data."
^STRUCTURE = "FIPS_EQ.FMT"
END_OBJECT = TABLE
END
The FIPS Pixel Field of View data lists the FOV pixels.
PDS_VERSION_ID = "PDS3"
/* ** FILE FORMAT ** */
FILE_RECORDS = 931
RECORD_TYPE = FIXED_LENGTH
RECORD_BYTES = 88
/* ** GENERAL DATA DESCRIPTION PARAMETERS ** */
PRODUCT_ID = "FIPA_F2004216CDR_V1"
PRODUCT_VERSION_ID =
"01"
PRODUCT_CREATION_TIME =
2014-06-04T10:00:00
PRODUCT_TYPE = ANCILLARY
STANDARD_DATA_PRODUCT_ID =
"FIPS_FOVPIXEL"
SOFTWARE_NAME = "mcpmapgen"
SOFTWARE_VERSION_ID =
"1.0"
INSTRUMENT_HOST_NAME =
"MESSENGER"
INSTRUMENT_NAME = "ENERGETIC PARTICLE AND PLASMA SPECTROMETER"
INSTRUMENT_ID = "EPPS"
DATA_SET_ID =
"MESS-E/V/H/SW-EPPS-3-FIPS-CDR-V1.0"
DATA_SET_NAME = "MESSENGER E/V/H/SW EPPS CALIBRATED FIPS
CDR
V1.0"
START_TIME = 2004-08-03T00:00:00
STOP_TIME = 2008-08-17T23:59:59
^HEADER = ("FIPA_F2004216CDR_V1.TAB", 1)
^ASCII_TABLE = ("FIPA_F2004216CDR_V1.TAB", 5)
OBJECT = HEADER
HEADER_TYPE = TEXT
INTERCHANGE_FORMAT
= "ASCII"
RECORDS = 4
BYTES = 352
DESCRIPTION =
"The first four records of this
file are
the header section. The header contains column
headings
to improve usability."
END_OBJECT = HEADER
OBJECT = ASCII_TABLE
COLUMNS = 7
INTERCHANGE_FORMAT
= ASCII
ROW_BYTES
= 88
ROWS =
927
DESCRIPTION =
"
This table contains normalizations for the FOV
pixels."
^STRUCTURE
= "FIPS_FOVPIXEL.FMT"
END_OBJECT = ASCII_TABLE
END
The EPPS CDR data products are constructed according to the data object concepts developed by the PDS. By adopting the PDS format, the data products are consistent in content and organization with other planetary data collections. In the PDS standard, the CDR data file is grouped into objects with PDS labels describing the objects. Each CDR data product consists of two files:
One of the time fields in the FIPS table objects reference the Mission Elapsed Time (MET). This MET is the spacecraft time in integer seconds that is transmitted to MESSENGER subsystems by the Integrated Electronics Module (IEM). This is referred to by the MESSENGER project as Mission Elapsed Time (MET). MET = 0 is August 3, 2004, at 05:59:16 UTC (coordinated universal time), which is 1000 seconds prior to the MESSENGER launch. Relativistic effects and circumstances occurring during the mission would result in MET not being a true account of seconds since launch. Following a planned spacecraft clock reset in early 2013, partition numbers (1/, or 2/) were added to product labels to disambiguate MET seconds after the spacecraft clock reset (if partition number is not present, SPICE defaults to partition 1/). For this reason the MESSENGER spacecraft clock coefficients file is archived at the PDS Navigation and Ancillary Information Facility (NAIF) Node. This file is used in conjunction with the leapseconds kernel file in order to calculate the conversion between MET and UTC.
The conversion is easily done through the use of SPICE kernels and the CHRONOS Utility. CHRONOS is a utility included with the SPICE package that is distributed by the PDS NAIF node. The SPICE kernels are files that contain the information needed to perform the conversion. Two SPICE kernels are required. One is the Leapseconds Kernel (LSK) and the other is the MESSENGER Spacecraft Clock Kernel (SCLK). The SCLK file is used by CHRONOS to convert between spacecraft clock time and ephemeris time, while the LSK file is used to convert from ephemeris time to UTC time. The CHRONOS utility is self-documenting and the SPICE package itself contains full documentation on each of the utilities (including CHRONOS) and how they are used.
EPPS CDR data is time-tagged with spacecraft event time (SCET) in the following UTC format: CCYY-DDDTHH:MM:SS.sss. This format represents a concatenation of the conventional date and time expressions with the two parts separated by the letter T:
CC - century (00-99)
YY - year (00-99)
DDD - day of year (001-366)
T - date/time separator
HH - hour (00-23)
MM - minute (00-59)
SS - second (00-59)
sss - fractions of second (000-999)
There are two coordinate systems
in use in the EPPS CDR data products: 1) the Mercury-centric Solar Orbital
(MSO, defined in the MESSENGER SPICE Dynamic Frames Kernel) used for spacecraft
position vectors; and 2) the FIPS Spherical coordinate system, used for
FIPS incident angles since it represents natural coordinates for the sensor. The latter is a
spherical version of the FIPS Cartesian coordinate system which is defined in
the MESSENGER SPICE Frames Kernel
FIPS Spherical coordinates consist of a radius (r), zenith angle (theta)
and azimuthal angle (phi), The zenith
angle is defined as the angle between the vector and the z axis in the FIPS
Cartesian coordinate system. It ranges
from 0 to 180 degrees. The azimuthal
angle ranges from 0 to 360 degrees and is defined as the angle between the
vector and the x axis in the FIPS Cartesian coordinate system. The radius is defined as usual as the
magnitude of the FIPS Cartesian vector.
The data are organized following PDS standards and stored on
hard disk at the MESSENGER SOC. The SOC will transfer data to PDS via
electronic transfer and delivery methods as detailed in section 5.3.3.
After verification of the data transfer PDS will provide public access to
MESSENGER science data products through its online data distribution system.
The EPPS CDR data archive volume set will include all data acquired during the MESSENGER mission. The archive validation procedure described in this section applies to data products generated during all post launch phases of the mission. To be clear, there is one and only one documentation volume and one and only one EPPS CDR data archive volume created over the whole mission. Release dates are stated in the schedule in [2]. Updates to the CDR data volume will occur according to the same schedule. Updates to the documentation volume will occur at the discretion of the EPPS team.
PDS standards recommend that all data included in the formal archive be validated through a peer-review process. This process is designed to ensure that both the data and documentation are of sufficient quality to be useful to future generations of scientists. The schedule of PDS data deliveries, however, necessitate some modification of the normal PDS review process since it is impractical to convene a review panel to examine the archive volume for every PDS data delivery. The following describes the modified validation process. The process is presented as several steps, most of which occur in the PDS peer review. This peer review is conducted before any volumes are produced and released to PDS.
The peer review panel consists of members of the EPPS team, the PPI node of PDS, and at least one outside scientist actively working in the field of energetic particles research. The PDS personnel are responsible for validating that the volumes are fully compliant with PDS standards. The instrument team and outside reviewer(s) are responsible for verifying the content of the data set, the completeness of the documentation, and the usability of the data in its archive format.
The peer review will validate the documentation and data archive volumes via a two step process. First the panel reviews this document and verifies that the volumes and CDRs produced to this specification will be useful. Next the panel reviews the initial release of the data and documentation volumes to verify that the volumes meet this specification and are acceptable. Once automated production begins, software provided by APL produce a summary of each data product and software provided by the PPI node verifies that all the files required by PDS are present and the files themselves conform to PDS standards. If an error is detected by either of the above programs, the error is corrected, if possible, before the update to the volume is delivered. Otherwise the correction will occur at the next scheduled delivery date. If an error in a data file is uncorrectable, (i.e. an error in the downlink data file) the error is described in the cumulative errata file that is included in the data archive volume.
The peer review will also validate the EPPS CDR data in a two step process. The first step consists of reviewing a sample data set for compliance with the PDS standards. The sample data set is delivered and reviewed in conjunction with delivery and review of this SIS document. The second step is examination of the data to ensure usability and completeness. The PDS personnel will be responsible for validating that the CDR data set is fully compliant with PDS standards. The instrument team and the outside science reviewer(s) will be responsible for verifying the content of the data set, the completeness of the documentation, and the usability of the data in its archive format.
Any deficiencies in the archive data or documentation volumes will be recorded as liens against the product by the review panel. The sample data set is created using software provided by APL. Once the sample data are validated, and all liens placed against the product or product generation software are resolved, the same software will be used to generate subsequent data products in an automated fashion.
Once automated production begins, the data file content will
be spot checked by members of the EPPS team. “Quick look” products generated by
software provided by ACT and the EPPS team will be produced routinely and examined
by members of the team. In addition, the data will be actively used by team
members to perform their analysis. Any discrepancies in the data noted during
these activities will be investigated. If the discrepancy is a data error, the
response will depend on the source of the error. If the error is in the
software producing the data product, the error will be corrected and the data
affected will be reproduced, replacing the data file. If there is a correctable
error in a data file, the file will be replaced. If an error in a data file is
uncorrectable, the error will be described in the cumulative errata file
included in the archive volume. The structure of data files and labels will be
spot checked by the PPI node for compliance with PDS standards and this SIS.
The MESSENGER EPPS CDR data products will be archived at the PDS PPI Node. The automated production and release of CDRs lends itself to the regular release schedule outlined in [2]. If errors are discovered the data will be replaced with corrected CDRs on the next scheduled delivery date.
Calibration tables and calibration procedures will be required to properly analyze CDRs. These ancillary data will be archived at the PDS PPI Node as part of the EPPS documentation volume. The documentation volume is referenced by all EPPS data archive volumes. The documentation volume will therefore include both the EPPS EDR SIS and the EPPS CDR SIS in addition to the calibration tables, calibration procedures, and other documents applicable to either data archive volume. A first release of the EPPS documentation volume accompanied the initial release of the EPPS EDR data archive. An update to the EPPS documentation volume will accompany the initial release of the CDR data archive. After the initial release of the CDR level documentation there will be updates to the documentation volume whenever the EPPS team determines that they have a sufficiently improved calibration to warrant a new release.
The possibility exists that errors may be introduced into the archive even with validation procedures applied to the archive volumes. An ERRATA report file is maintained to track and document all discovered uncorrectable errors that may occur during the mission. Correctable errors, such as revised CDRs or CDRs that were missing from a previous PDS delivery will be provided at the next scheduled PDS delivery or at the final delivery date (schedule in [2]). PDS will then replace the outdated files with the revised CDR files in the data directories of the archive volume. File revisions are also recorded in the data product label keywords PRODUCT_VERSION_ID and PRODUCT_CREATION_TIME, which can be used in addition to ERRATA.TXT to detect updates. The ERRATA report file is archived in the ROOT directory of the EPPS CDR data volume.
Data are stored in ASCII table
format. A detached PDS label file will provide a detailed description of the
structure of each table.
The following are the keyword
definitions for the detached PDS label file, which accompanies the instrument
data file. The detached PDS label file
has the same name as the data file it describes, except for the extension .LBL
to distinguish it as a label file.
PDS_VERSION_ID
Represents the version number
of the PDS standards documents that is valid when a data product label is
created. PDS3 is used for the MESSENGER data products.
FILE_RECORDS
Indicates the number of physical
file records, including both label records and data records.
RECORD_TYPE
Indicates the record format of
a file. Note: In the PDS, when record_type is used in a
detached label file it always describes its corresponding detached data file,
not the label file itself. The use of
record_type along with other file-related data elements is fully described in
the PDS Standards Reference.
RECORD_BYTES
Indicates the number of bytes
in a physical file record, including record terminators and separators. Note:
In the PDS, the use of record_bytes, along with other file-related data
elements is fully described in the Standards Reference.
PRODUCT_ID
Represents a permanent, unique
identifier assigned to a data product by its producer.
PRODUCT_CREATION_TIME
Defines the UTC system format
time when a product was created.
PRODUCT_VERSION_ID
Identifies the version of an
individual product within a data set.
Example: 1.0, 2.0, 3.0.
Product_version_id will be
incremented if a given CDR has to be regenerated and sent to PDS to replace a
previously submitted CDR.
PRODUCT_TYPE
Identifies the type or category
of a product within a data set.
STANDARD_DATA_PRODUCT_ID
Used to link an EPPS CDR file
to one of the 12 types of EPPS data products
defined within the EPPS CDR SIS.
SOFTWARE_NAME
Identifies the data processing
software used to convert from spacecraft telemetry into CDR products.
SOFTWARE_VERSION_ID
Indicates the version of the
data processing software used to generate the CDR products from the EDRs.
MD5_CHECKSUM
Used to verify the successful
electronic transfer of the CDR from the SOC to the PDS-PPI Node.
INSTRUMENT_HOST_NAME
The full name of the host on
which an instrument is based. In this
case it is the MESSENGER spacecraft.
INSTRUMENT_NAME
Provides the full name of the
instrument.
INSTRUMENT_ID
Provides an abbreviated name or
acronym which identifies an instrument.
DATA_SET_ID
The data_set_id element is a
unique alphanumeric identifier for a data set or a data product. The
data_set_id value for a given data set or product is constructed according to
flight project naming conventions. There
is only one data_set_id for the EPPS CDRs.
MISSION_PHASE_NAME
Provides the commonly used
identifier of a mission phase.
TARGET_NAME
The target_name element identifies a target. The target may be a planet,
satellite,ring,region, feature,
asteroid or comet.
START_TIME
Provides the date and time of
the beginning of an event or observation (whether it be a spacecraft, ground-based, or system
event) in UTC system format.
STOP_TIME
Provides the date and time of
the end of an observation or event (whether it be a spacecraft, ground-based,
or system event) in UTC system format.
SPACECRAFT_CLOCK_START_COUNT
Provides the value of the
spacecraft clock at the beginning of a time period of interest.
SPACECRAFT_CLOCK_STOP_COUNT
Provides the value of the
spacecraft clock at the end of a time
period of interest.
^TABLE
Pointer to the CDR file which
contains the data in ASCII table format. The structure of the data file is
defined in a referenced format file.
OBJECT
Specifies that the CDR is a PDS
TABLE object. This object contains its own elements, which are defined below.
NOTE: the end of the object definition is always marked with an END_OBJECT line.
COLUMNS
Identifies the number of
columns (fields) in the table.
INTERCHANGE_FORMAT
This element specifies that the
table is in ASCII format.
ROW_BYTES
Specifies the number of bytes
for each row in the table.
ROWS
Identifies the number of rows
(records) in the table.
^STRUCTURE
This is a pointer to the
external file which provides the structure definition for the table object.
The following describes the
keywords used to describe the PDS Table Object. These keywords are contained in
the FORMAT (.FMT) files for each CDR data product.
COLUMN_NUMBER
Identifies the location of the
column within the larger data object (such as a table). For tables consisting
of rows (I= 1, N) and columns (j = 1, M) the column_number is the j-th index of
any row.
NAME
Indicates a literal value
representing the common term used to identify an element or object. NOTE: in
the PDS data dictionary, name is restricted to 30 characters and must conform
to PDS nomenclature standards.
BYTES
Specifies the number of bytes
allocated for this particular column element.
DATA_TYPE
Specifies the internal
representation and/or mathematical properties of the value being stored in this
column.
START_BYTE
Identifies the location of the
first byte of the particular column, counting from 1.
ITEMS
Defines the number of multiple,
identical occurrences of a single object. Used mainly in columns containing
spectral or histogram data.
ITEM_BYTES
The size in bytes of individual
items in a column. ITEMS * ITEM_BYTES should equal the value in the BYTES
column.
The format file will contain the
full text for describing each column of the table. See Appendices for a listing
of each field in the individual format files.
The file names developed for PDS data volumes are restricted to a maximum 27 character file name and a 3 character extension name with a period separating the file and extension names. Given this restriction the general form of the EPPS file name for CDRs will be “EEEZ_XYYYYDDDAAA_V#.TAB” where:
EEE instrument identifier: represents the EPPS instrument
EPS, EPPS/EPS
FIP, EPPS/FIPS
Z specifies whether the packet contains data taken from the high,
medium, or low priority science packet
A,
Ancillary Data (not from a packet)
H,
High Priority
M,
Medium Priority
L,
Low Priority
N,
Not Applicable
P,
Raw or Proton PHA packet
S,
data from Scan packet
The FSW6 upload removed the EPS PHA association with priority,
thus N indicates N/A association for EPS PHA CDRs
While FIPS PHA EDR data can extracted from several packet types,
these data are combined in the CDR product.
X specifies whether data contains PHA events, spectra/counts, rates, velocity distributions, or energy per charge table data.
P, PHA events
S, Spectra
R, Rates (i.e. Rate spectra)
V, Velocity distributions
E, E/q table
F, Pixel Field Of View table
NOTE: The FSW6
upload had the effect of retiring several CDRs and adding new ones. In order to
keep the EEEZ_XYYYYDDDAAA_V#.TAB file naming convention the Z and X characters
are used in conjunction to identify the new CDRs.
The values of Z_X
for each of the EPS and FIPS data products is shown below:
EPS High Priority Spectra: Z_X =
"H_S"
EPS Medium Priority Spectra: Z_X = "M_S"
EPS PHA: Z_X = "N_P"
EPS High Resolution Spectra: Z_X = "H_R"
EPS Low Resolution Spectra: Z_X = "L_R"
EPS Summary Spectra: Z_X = "S_S"
EPS Scan: Z_X = "S_R"
FIPS High Priority Spectra: Z_X = "H_S"
FIPS Medium Priority Spectra: Z_X =
"M_S"
FIPS PHA: Z_X = "P_P"
FIPS Scan : Z_X = "S_R"
FIPS HRPVD CDR: Z_X = "S_V"
FIPS E/q table: Z_X = "A_E"
YYYY four digit year
DDD three digit day of year
AAA specifies whether the data product is an EDR or CDR
V# Version number. The initial version is “V1”. The version number increments to “V2”, “V3”, etc for each successive version of the CDR product that is produced. A new version of the CDR product may be produced as a result of an error in the product or as a result of errors discovered in the product generation process.
TAB the file extension is dependent on the file type
.TAB, EPS and FIPS Instrument Data in ASCII table
.LBL, Detached PDS label file
Two archive volumes are created to archive both the EPPS CDR data and the documentation which will be needed to analyze the CDRs. The first volume is the EPPS Documentation Volume, having volume ID MESSEPPS_DOC. This documentation volume will contain products related to both the EPPS EDR and CDR data archives. The initial release of the documentation volume contains only EDR level documentation. CDR documents (such as the CDR SIS and dataset catalog) will be added to the volume at the time of initial release of those datasets. Once all of the EPPS data products are designed and released, the documentation volume will contain the following products:
The second archive volume, designated as the EPPS Data Archive Volume and having volume ID MESSEPPS_CDR, will contain the CDR data and required files for conforming to PDS volume archive standards. This includes the index files, AAREADME.TXT file, etc. The current best estimate of the data archive volume size is <TBD – data archive size> GB. This estimate was calculated by the MESSENGER project as part of a data downlink analysis for the entire mission.
The following illustration shows the directory structure
overview for the EPPS documentation volume. This volume will be periodically
updated as knowledge of the instrument, its calibration, and its operation
improve over time.
<ROOT>
______________________|______________________
| | | |
<CALIBRATION> <DOCUMENT> <CATALOG> <INDEX>
|
_____________|_____________
|
| |
<EDR_SIS>
<CDR_SIS> <DDR_SIS>
Figure 2 Documentation Volume Structure
<ROOT> Directory
This is the top-level volume directory.
The following are files contained in the root directory.
AAREADME.TXT
- General information file. Provides users with an overview of the contents and
organization of the associated volume, general instructions for its use, and
contact information.
VOLDESC.CAT - PDS file containing the VOLUME object. This
gives a high-level description of the contents of the volume. Information
includes: production date, producer name and institution, volume ID, etc.
ERRATA.TXT
- Text file for identifying and describing errors and/or anomalies found in the
current volume, and possibly previous volumes of a set. Any known errors for
the associated volume will be documented in this file.
<CALIBRATION> Directory
This will contain the calibration tables
needed to analyze the EPPS CDR data. The calibration tables are in ASCII
format. Format files for the calibration tables are also located here, as are
the following files.
CALINFO.TXT
– Brief description of the directory contents and naming conventions.
EPPS_*_EDR2CDR.PDF:
Describes the procedure used to convert
EDRs to CDRs for each instrument, (EPS or FIPS as indicated by the * text).
IMAGES: Directory containing image files
used by the HTML version of the EPPS_*_EDR2CDR documents.
FIP*.TAB: The
FIPS energy per charge and pixel field of view tables.
<CATALOG> Directory
This subdirectory contains the catalog
object files for the entire volume. The following files are included in the
catalog subdirectory.
CATINFO.TXT:
Identifies and describes the function of
each file in the catalog directory.
EPPS*DATASET.CAT:
Describes the general content of the EDR
data set for each instrument, as (indicated by the * text) and includes
information about the duration of the mission and the person or group
responsible for producing the data.
EPPS*DATASET_CDR.CAT:
Describes the general content of the CDR
data set for each instrument, (as indicated by the * text) and includes
information about the duration of the mission and the person or group responsible
for producing the data.
INSTRUMENT.CAT:
Describes physical attributes of the EPPS instrument and provides relevant
references to published literature.
INSTHOST.CAT:
Describes the MESSENGER spacecraft.
MISSION.CAT:
Describes the scientific goals and objectives of the MESSENGER program. It also
identifies key people and institutions.
PERSON.CAT:
Lists and provides contact information for the people involved in the MESSENGER
mission, including those involved with EPPS.
REF.CAT:
Provides references to scientific papers and other publications of interest to
those using the data, both for EPPS and the mission as a whole.
< DOCUMENT > Directory
This subdirectory contains the
documentation that will be needed in order to understand and analyze the EDR and
CDR data volumes. The documents will be separated into individual
subdirectories according to the document type. The document types are not
restricted to the four shown in the graphical depiction of the directory
structure. There will be as many document types as needed to categorize each
document. The following file is included in the subdirectory.
DOCINFO.TXT:
Identifies and describes the function of
each file in the DOCUMENT directory.
< INDEX > Directory
This subdirectory contains the MD5.TAB file,
which contains MD5 hash values for the volume.
MD5.TAB/.LBL:
Contains the MD5 hash values and label
information.
<ROOT>
___________________________|__________________________
| | | |
<DATA> <GEOMETRY> <INDEX> <LABEL>
|
____|______________________________________________________________________
| | |
| | | | |
| | <EPS_HI_SPECTRA> | <EPS_MED_SPECTRA> | <EPS_SUMMARY_SPECTRA> |
| | | | |
| <EPS_PHA>
<EPS_HIRES_SPECTRA>
<EPS_LORES_SPECTRA>
<EPS_SCAN_SPECTRA>
_|________________________________________________________________________
| | | | |
<FIPS_HI_SPECTRA>
<FIPS_MED_SPECTRA> | <FIPS_HIRES_PROTON_V> |
| |
<FIPS_SCAN> <FIPS_PHA>
|
|
<2008>
Figure 3 Data Volume Directory
Structure
<ROOT>
Directory
This is
the top-level directory of a volume. The following are files contained in the
root directory.
AAREADME.TXT - General information file. Provides users with
an overview of the contents and organization of the associated volume, general
instructions for its use, and contact information.
VOLDESC.CAT - PDS
file containing the VOLUME object. This gives a high-level description of the
contents of the volume. Information includes: production date, producer name
and institution, volume ID, etc.
ERRATA.TXT - Text file for identifying and describing
errors and/or anomalies found in the current volume, and possibly previous
volumes of a set. Any known errors for the associated volume will be documented
in this file. This includes revised CDRs
meant to replace CDRs in a previous PDS delivery.
<DATA>
Directory
This top level
directory contains the CDR data products. Directly underneath the <DATA>
directory are subdirectories corresponding to the nine standard data products
(section 5.2). The
directories are further subdivided into YEAR and MONTH directories.
<GEOMETRY>
Directory
This
subdirectory contains information about the files (e.g. SPICE kernels, etc)
needed to describe the observation geometry for the data.
GEOMINFO.TXT : Identifies
and describes the SPICE kernels that a user must have in order to determine observation
geometry for the data. The SPICE kernel files are archived with the PDS NAIF
node.
<INDEX>
Directory
This
subdirectory contains the indices for all data products on the volume. The following files are contained in the
index subdirectory.
INDXINFO.TXT – Identifies and describes the function
of each file in the index subdirectory.
This includes a description of the structure and contents of each index
table in the subdirectory AND usage notes.
INDEX.TAB - The CDR index file is organized as a table:
there is one entry for each of the data files included in the EPPS data set;
the columns contain parameters that describe the observation and instrument and
spacecraft parameters. These parameters include state information, such as
integration time, spacecraft clock count, time of observation, and instrument
modes.
INDEX.LBL - Detached PDS label for INDEX.TAB. It contains
the INDEX_TABLE object which identifies and describes the columns of the EPPS
index table.
MD5.TAB - The MD5 checksum file that contains MD5 hash values for every
file in the volume.
MD5.LBL - Detached PDS label for MD5.TAB.
<LABEL>
Directory
This
subdirectory contains the “label fragments” (i.e., the *.FMT files) for all data products on the volume. These format files describe the table and
data objects which store the data.
The MESSENGER EPPS data and volume archives will be transferred from the SOC to the PDS PPI Node using the electronic transfer process detailed in section 5.3.3. The SPICE kernels will be electronically transferred to the NAIF node. The transfer will take place according to the schedule in [2].
The following are the columns as
defined by the EPSHIGH_CDR.FMT structure file. This file defines the ASCII
table containing the EPS High Priority spectra data. Archive volume is
optimized by defining the table structure once and providing a reference to it
in the PDS label file. The columns are numbered according to their column order
in the table. Data_Type refers to the
PDS standards data type for a particular column in the table.
The FSW6 upload was done on
8/18/2008 and implemented on 8/19/2008. The software update retired the EPS
High Priority Spectra packet. Thus there are no EPS Hi Spectra CDRs on or after
8/19/2008.
Table 20 EPSHIGH_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Column Name |
Summary (see full text for column description) |
|
21 |
TIME |
TIME |
Spacecraft event time (UTC)
for this data record. |
|
23 |
ASCII Integer |
ACCUM_TIME |
The time period over which
the rates were accumulated. (Seconds) |
|
23 |
ASCII Real |
RADIAL_DIST |
The distance of the
spacecraft from Mercury. (Mercury radii) |
|
23 |
ASCII Real |
MSO_LOCAL_TIME |
The Mercury longitude of
the spacecraft. (Fractional Hours) |
|
23 |
ASCII Real |
MSO_LATITUDE |
The Mercury latitude of the
spacecraft. (Degrees) |
|
23 |
ASCII Real |
MSGR_MSO_X |
The X position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Y |
The Y position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Z |
The Z position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23x8 |
ASCII Real |
ION_S00_RATES |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S00_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S01_RATES |
Ion count rate spectrum for
ion direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S01_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S02_RATES |
Ion count rate spectrum for
ion direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S02_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S03_RATES |
Ion count rate spectrum for
ion direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S03_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S04_RATES |
Ion count rate spectrum for
ion direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S04_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S05_RATES |
Ion count rate spectrum for
ion direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S05_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S00_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S00_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S01_FLUX |
Ion count rate spectrum for
ion direction 1, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S01_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S02_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S02_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S03_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S03_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S04_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S04_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S05_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S05_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_RATES |
Coarse electron count rate
spectrum for electron direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_RATES |
Coarse electron count rate
spectrum for electron direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_RATES |
Coarse electron count rate
spectrum for electron direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_RATES |
Coarse electron count rate
spectrum for electron direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_RATES |
Coarse electron count rate
spectrum for electron direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_RATES |
Coarse electron count rate
spectrum for electron direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_FLUX |
Coarse electron flux spectrum
for electron direction 1, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x12 |
ASCII Real |
FAST_ENERGY_RATE |
The 12 fast energy hardware
count rates. (counts/sec) |
|
23x12 |
ASCII Real |
SHAPED_ENERGY_RATE |
The 12 shaped energy
hardware count rates. (counts/sec) |
|
23 |
ASCII Real |
E_EVENT_RATE |
Electron event hardware
count rate. (counts/sec) |
|
23 |
ASCII Real |
ION_EVENT_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
E_PROCESSED_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
ION_PROCESSED_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
PILEUP_E_DISCARD_RATE |
Rate of electron events
discarded due to pileup condition. (counts/sec) |
|
23 |
ASCII Real |
MULTIPLE_E_HITS_DISCARD_RATE |
Rate of electron events
discarded due to multiple hits. (counts/sec) |
|
23 |
ASCII Real |
PILEUP_ION_DISCARD_RATE |
Rate of ion events discarded
due to pileup condition. (counts/sec) |
|
23 |
ASCII Real |
MULTIPLE_ION_HITS_DISCARD_RATE |
Rate of ion events
discarded due to multiple hits. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 0. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 0.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 0. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 0.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 1. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 1.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 1. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 1.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 2. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 2.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 2. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 2.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 3. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 3.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 3. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 3.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 4. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 4.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 4. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 4.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 5. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 5.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 5. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 5.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 0. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 0. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 0. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 0. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 1. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 1. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 1. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 1. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 2. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 2. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 2. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 2. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 3. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 3. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 3. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 3. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 4. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 4. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 4. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 4. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 5. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 5. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 5. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 5. (1/cm^s
sr keV sec) |
1.
TIME
Spacecraft event time (UTC) for this data record.
2.
ACCUM_TIME
The length of the accumulation interval for this data record.
3.
RADIAL_DIST
The distance of the spacecraft from Mercury in the MSO frame, in
units of Mercury radii..
4.
MSO_LOCAL_TIME
The Mercury longitude of the spacecraft expressed in fractional
hours.
5.
MSO_LATITUDE
The Mercury latitude of the spacecraft in degrees.
The X position of
the spacecraft in the MSO frame, in units of Mercury radii.
The Y position of
the spacecraft in the MSO frame, in units of Mercury radii.
The Z position of
the spacecraft in the MSO frame, in units of Mercury radii.
9.
ION_Sn_RATES
Ion rate (counts/second) histogram for ion direction n (SSD
detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that define
the entire 160 degree field of view of the sensor for ions, and each
representing about 27 degrees out of the entire field of view. Histogram
contains the 8 bins shown in Table 4 and Table 6.
10.
ION_Sn_RATES_UNC
Uncertainties for the ION_Sn_RATES.
11.
ION_Sn_FLUX
Ion flux (1/cm2 sr keV sec) histogram for ion direction
n (SSD detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that
define the entire 160 degree field of view of the sensor for ions, and each representing
about 27 degrees out of the entire field of view. Histogram contains the 8 bins shown in Table 4 and Table 6.
12.
ION_Sn_FLUX_UNC
Uncertainties for the ION_Sn_FLUX.
13.
COARSE_E_Sn_RATES
Electron rate (counts/second) histogram for electron direction n
(SSD detector n*2), which is 1 of the 6 electron directions (0 through 5) that
define the entire 160 degree field of view of the sensor for electrons, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 8 bins shown in Table 5 and Table 7.
14.
COARSE_E_Sn_RATES_UNC
Uncertainties for the COARSE_E_Sn_RATES.
15.
COARSE_E_Sn_FLUX
Electron flux (1/cm2 sr keV sec) histogram for electron
direction n (SSD detector n*2), which is 1 of the 6 ion directions (0 through
5) that define the entire 160 degree field of view of the sensor for ions, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 8 bins shown in Table 4 and Table 6.
16.
COARSE_E_Sn_FLUX_UNC
Uncertainties for the COARSE_E_Sn_FLUX.
17.
FAST_ENERGY_RATE
Fast energy hardware counter from one of 12 Solid State Detectors
that define the 160 degree sensor field of view for both electrons and
ions. All even-numbered SSDs are
electrons and all odd channels are ions.
This channel is the rate (counts/sec) of pulses whose amplitude is used
to determine the energy of the particle that generated the pulse.
18.
SHAPED_ENERGY_RATE
Shaped energy hardware counter from one of 12 Solid State
Detectors that define the 160 degree sensor field of view for both electrons
and ions. All even-numbered SSDs are
electrons and all odd channels are ions.
This channel is the rate (counts/sec) of pulses whose amplitude is used
to determine the energy of the particle that generated the pulse.
19.
E_EVENT_RATE
Hardware rate (counts/sec) for all classified Electron events
registered in the fast processing electronics upstream from the Event
Processing Computer. Because the Event Processing Computer can process at most
about 5000 events, this counter allows the user to renormalize the processed
output rates to retrieve true intensities.
20.
ION_EVENT_RATE
Hardware rate (counts/sec) for all classified Ion events
registered in the fast processing electronics upstream from the Event
Processing Computer. Because the Event Processing Computer can process at most
about 5000 events, this counter allows the user to renormalize the processed
output rates to retrieve true intensities.
21.
E_PROCESSED_RATE
22.
ION_PROCESSED_RATE
Rate of high energy ion events processed by the Event Processing
Computer during the accumulation interval.
23.
PILEUP_E_DISCARD_RATE
Rate of electron events discarded by the Event Processing Computer
due to pileup condition.
24.
MULTIPLE_E_HITS_DISCARD_RATE
Rate of electron events
discarded by the Event Processing Computer due to multiple electron hits.
25.
PILEUP_ION_DISCARD_RATE
Rate of high energy ion
events discarded by the Event Processing Computer due to pileup condition.
26.
MULTIPLE_ION_DISCARD_RATE
Rate of high energy ion
events discarded by the Event Processing Computer due to multiple ion hits.
27.
FINE_E_S0nB0m_RATE
A series of 10 count rates
(counts/sec) for “super bin m” for
electron direction n (SSD detector 2*n), which is 1 of the 6 electron
directions (numbered 0 through 5) that define the entire 160 degree field of
view of the sensor, and each representing about 27 degrees out of the entire
field of view. Each super bin is the
accumulation of a subset of bin counts in one 1/10 *(ACCUM_TIME) subinterval.
Super bin 0 is the sum of the energy bins 0-3 shown in Table 5 and Table 7. Super bin 1 is the sum of bins 4-7 shown
in Table 5 and Table 7. Each super bin pair is measured once per
subinterval for 10 subintervals, making a total of 20 items.
28.
FINE_E_S0nB0m_RATE_UNC
Uncertainties for FINE_E_S0nB0m_RATE
29.
FINE_E_S0nB0m_FLUX
A series of 10 count rates
(1/cm^2 sr keV sec) for “super bin m”
for electron direction n (SSD detector 2*n), which is 1 of the 6 electron
directions (numbered 0 through 5) that define the entire 160 degree field of
view of the sensor, and each representing about 27 degrees out of the entire
field of view. Each super bin is the
accumulation of a subset of bin counts in one 1/10*(ACCUM_TIME) subinterval.
Super bin 0 is the sum of the energy bins 0-3 shown in Table 5 and Table 7. Super bin 1 is
the sum of bins 4-7 shown in Table 5 and Table 7. Each super bin
pair is measured once per subinterval for 10 subintervals, making a total of 20
items.
30.
FINE_E_S0nB0m_FLUX_UNC
Uncertainties for FINE_E_S0nB0m_FLUX
The following are the columns as
defined by the EPSMED_CDR.FMT structure file. This file defines the ASCII table
containing the EPS Medium Priority spectra data. Archive volume is optimized by
defining the table structure once and providing a reference to it in the PDS
label file. The columns are numbered according to their column order in the
table. Data_Type refers to the PDS
standards data type for a particular column in the table.
The FSW6 upload was done on 8/18/2008 and implemented on 8/19/2008. The software update retired the EPS Medium Priority Spectra packet. Thus there are no EPS Medium Priority CDRs on or after 8/19/2008.
Table 21
EPSMED_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Column Name |
Summary (see full text for column description) |
|
21 |
TIME |
TIME |
Spacecraft event time (UTC)
for this data record. |
|
23 |
ASCII Integer |
ACCUM_TIME |
The time period over which
the rates were accumulated. (Seconds) |
|
23 |
ASCII Real |
RADIAL_DIST |
The distance of the
spacecraft from Mercury. (Mercury radii) |
|
23 |
ASCII Real |
MSO_LOCAL_TIME |
The Mercury longitude of
the spacecraft. (Fractional Hours) |
|
23 |
ASCII Real |
MSO_LATITUDE |
The Mercury latitude of the
spacecraft. (Degrees) |
|
23 |
ASCII Real |
MSGR_MSO_X |
The X position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Y |
The Y position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Z |
The Z position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23x8 |
ASCII Real |
ION_S00_RATES |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S00_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S01_RATES |
Ion count rate spectrum for
ion direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S01_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S02_RATES |
Ion count rate spectrum for
ion direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S02_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S03_RATES |
Ion count rate spectrum for
ion direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S03_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S04_RATES |
Ion count rate spectrum for
ion direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S04_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S05_RATES |
Ion count rate spectrum for
ion direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S05_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
ION_S00_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S00_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S01_FLUX |
Ion count rate spectrum for
ion direction 1, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S01_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S02_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S02_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S03_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S03_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S04_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S04_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S05_FLUX |
Ion count rate spectrum for
ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
ION_S05_FLUX_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_RATES |
Coarse electron count rate
spectrum for electron direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 0, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_RATES |
Coarse electron count rate
spectrum for electron direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 1, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_RATES |
Coarse electron count rate
spectrum for electron direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 2, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_RATES |
Coarse electron count rate
spectrum for electron direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 3, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_RATES |
Coarse electron count rate
spectrum for electron direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 4, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_RATES |
Coarse electron count rate
spectrum for electron direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_RATES_UNC |
Coarse electron count rate
spectrum uncertainty for electron direction 5, 8 energy bins. (counts/sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S00_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_FLUX |
Coarse electron flux
spectrum for electron direction 1, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S01_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S02_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S03_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S04_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_FLUX |
Coarse electron flux
spectrum for electron direction 0, 8 energy bins. (1/cm^2 sr keV sec) |
|
23x8 |
ASCII Real |
COARSE_E_S05_FLUX_UNC |
Coarse electron flux
spectrum uncertainty for electron direction 0, 8 energy bins. (1/cm^2 sr keV
sec) |
|
23x12 |
ASCII Real |
SHAPED_ENERGY_RATE |
The 12 shaped energy
hardware count rates. (counts/sec) |
|
23 |
ASCII Real |
E_EVENT_RATE |
Electron event hardware
count rate. (counts/sec) |
|
23 |
ASCII Real |
ION_EVENT_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
E_PROCESSED_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
ION_PROCESSED_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
PILEUP_E_DISCARD_RATE |
Rate of electron events
discarded due to pileup condition. (counts/sec) |
|
23 |
ASCII Real |
MULTIPLE_E_HITS_DISCARD_RATE |
Rate of electron events
discarded due to multiple hits. (counts/sec) |
|
23 |
ASCII Real |
PILEUP_ION_DISCARD_RATE |
Rate of ion events
discarded due to pileup condition. (counts/sec) |
|
23 |
ASCII Real |
MULTIPLE_ION_HITS_DISCARD_RATE |
Rate of ion events
discarded due to multiple hits. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 0. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 0.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 0. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 0.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 1. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 1.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 1. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 1.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 2. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 2.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 2. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 2.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 3. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 3.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 3. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 3.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 4. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 4.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 4. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 4.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_RATE |
Ten sub-sampled electron
count rates, super bin 0 from electron direction 5. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 0 from electron direction 5.
(counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_RATE |
Ten sub-sampled electron
count rates, super bin 1 from electron direction 5. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_RATE_UNC |
Uncertainties for ten
sub-sampled electron count rates, super bin 1 from electron direction 5. (counts/sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 0. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 0. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 0. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S00B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 0. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 1. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B00_FLUX_UNC |
Uncertainties for ten sub-sampled
electron fluxes, super bin 0 from electron direction 1. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 1. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S01B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 1. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 2. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 2. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 2. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S02B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 2. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 3. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 3. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 3. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S03B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 3. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 4. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 4. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 4. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S04B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 4. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_FLUX |
Ten sub-sampled electron
fluxes, super bin 0 from electron direction 5. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B00_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 0 from electron direction 5. (1/cm^s
sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_FLUX |
Ten sub-sampled electron
fluxes, super bin 1 from electron direction 5. (1/cm^s sr keV sec) |
|
23x10 |
ASCII Real |
FINE_E_S05B01_FLUX_UNC |
Uncertainties for ten
sub-sampled electron fluxes, super bin 1 from electron direction 5. (1/cm^s
sr keV sec) |
1.
TIME
Spacecraft event time (UTC) for this data record.
2.
ACCUM_TIME
The length of the accumulation interval for this data record.
3.
RADIAL_DIST
The distance of the spacecraft from Mercury in the MSO frame, in
units of Mercury radii..
4.
MSO_LOCAL_TIME
The Mercury longitude of the spacecraft expressed in fractional
hours.
5.
MSO_LATITUDE
The Mercury latitude of the spacecraft in degrees.
6.
MSGR_MSO_X
The X position of
the spacecraft in the MSO frame, in units of Mercury radii.
7.
MSGR_MSO_Y
The Y position of
the spacecraft in the MSO frame, in units of Mercury radii.
8.
MSGR_MSO_Z
The Z position of
the spacecraft in the MSO frame, in units of Mercury radii.
9.
ION_Sn_RATES
Ion rate (counts/second) histogram for ion direction n (SSD
detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that define
the entire 160 degree field of view of the sensor for ions, and each
representing about 27 degrees out of the entire field of view. Histogram contains the 8 bins shown in Table 4 and Table 6.
10.
ION_Sn_RATES_UNC
Uncertainties for the ION_Sn_RATES.
11.
ION_Sn_FLUX
Ion flux (1/cm2 sr keV sec) histogram for ion direction
n (SSD detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that
define the entire 160 degree field of view of the sensor for ions, and each
representing about 27 degrees out of the entire field of view. Histogram contains the 8 bins shown in Table 4 and Table 6.
12.
ION_Sn_FLUX_UNC
Uncertainties for the ION_Sn_FLUX.
13.
COARSE_E_Sn_RATES
Electron rate (counts/second) histogram for electron direction n
(SSD detector n*2), which is 1 of the 6 electron directions (0 through 5) that
define the entire 160 degree field of view of the sensor for electrons, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 8 bins shown in Table 5 and Table 7.
14.
COARSE_E_Sn_RATES_UNC
Uncertainties for the COARSE_E_Sn_RATES.
15.
COARSE_E_Sn_FLUX
Electron flux (1/cm2 sr keV sec) histogram for electron
direction n (SSD detector n*2), which is 1 of the 6 ion directions (0 through
5) that define the entire 160 degree field of view of the sensor for ions, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 8 bins shown in Table 5 and Table 7.
16.
COARSE_E_Sn_FLUX_UNC
Uncertainties for the COARSE_E_Sn_FLUX.
17.
SHAPED_ENERGY_RATE
Shaped energy hardware counter from one of 12 Solid State
Detectors that define the 160 degree sensor field of view for both electrons
and ions. All even-numbered SSDs are
electrons and all odd channels are ions.
This channel is the rate (counts/sec) of pulses whose amplitude is used
to determine the energy of the particle that generated the pulse.
18.
E_EVENT_RATE
Hardware rate (counts/sec) for all classified Electron events
registered in the fast processing electronics upstream from the Event
Processing Computer. Because the Event Processing Computer can process at most
about 5000 events, this counter allows the user to renormalize the processed
output rates to retrieve true intensities.
19.
ION_EVENT_RATE
Hardware rate (counts/sec) for all classified Ion events
registered in the fast processing electronics upstream from the Event
Processing Computer. Because the Event Processing Computer can process at most
about 5000 events, this counter allows the user to renormalize the processed
output rates to retrieve true intensities.
20.
E_PROCESSED_RATE
21.
ION_PROCESSED_RATE
Rate of high energy ion events processed by the Event Processing
Computer during the accumulation interval.
22.
PILEUP_E_DISCARD_RATE
Rate of electron events discarded by the Event Processing Computer
due to pileup condition.
23.
MULTIPLE_E_HITS_DISCARD_RATE
Rate of electron events
discarded by the Event Processing Computer due to multiple electron hits.
24.
PILEUP_ION_DISCARD_RATE
Rate of high energy ion
events discarded by the Event Processing Computer due to pileup condition.
25.
MULTIPLE_ION_DISCARD_RATE
Rate of high energy ion
events discarded by the Event Processing Computer due to multiple ion hits.
26.
FINE_E_S0nB0m_RATE
A series of 10 count rates
(counts/sec) for “super bin m” for
electron direction n (SSD detector 2*n), which is 1 of the 6 electron
directions (numbered 0 through 5) that define the entire 160 degree field of
view of the sensor, and each representing about 27 degrees out of the entire
field of view. Each super bin is the
accumulation of a subset of bin counts in one 1/10*(ACCUM_TIME) subinterval.
Super bin 0 is the sum of the energy bins 0-3 shown in Table 5 and Table 7. Super bin 1 is the sum of bins 4-7 shown
in Table 5 and Table 7. Each super bin
pair is measured once per subinterval for 10 subintervals, making a total of 20
items.
27.
FINE_E_S0nB0m_RATE_UNC
Uncertainties for FINE_E_S0nB0m_RATE
28.
FINE_E_S0nB0m_FLUX
A series of 10 count rates
(1/cm^2 sr keV sec) for “super bin m”
for electron direction n (SSD detector 2*n), which is 1 of the 6 electron
directions (numbered 0 through 5) that define the entire 160 degree field of
view of the sensor, and each representing about 27 degrees out of the entire
field of view. Each super bin is the
accumulation of a subset of bin counts in one 1/10*(ACCUM_TIME) subinterval.
Super bin 0 is the sum of the energy bins 0-3 shown in Table 5 and Table 7. Super bin 1 is the sum of bins 4-7 shown
in Table 5 and Table 7. Each super bin pair is measured once per
subinterval for 10 subintervals, making a total of 20 items.
29.
FINE_E_S0nB0m_FLUX_UNC
Uncertainties for FINE_E_S0nB0m_FLUX
The following are the columns as
defined by the EPS_PHA_CDR.FMT structure file. This file defines the ASCII
table containing the EPS Pulse Height Analysis (PHA) event data. The FSW6
upload resulted in changing the EPS PHA data format. It was decided to merge
the new format with the previously existing format rather than create an
entirely new CDR.
Prior to FSW6 the EPS PHA data
could be one of four types: Electron PHA event, Low Energy Ion PHA event, High
Energy Ion PHA event, Diagnostic PHA event. After FSW6 there are no separate
event types.
There are some common columns for
the PHA formats pre and post FSW6, however other columns may be unique. Columns
added as a result of FSW6 are INTEGRATION_TIME
and ENERGY_BIN. The EPS PHA ASCII table will contain all the possible columns
that may be populated and will include a “Not
Applicable” value when appropriate.
Archive volume is optimized by defining the table structure once and
providing a reference to it in the PDS label file. The columns are numbered
according to their column order in the table. Data_Type refers to the PDS
standards data type for a particular column in the table.
Table 22
EPS_PHA_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Column Name |
Summary (see full text for column description) |
|
21 |
TIME |
TIME |
Spacecraft event time (UTC)
for this data record. |
|
23 |
ASCII Real |
RADIAL_DIST |
The distance of the
spacecraft from Mercury. (Mercury radii) |
|
23 |
ASCII Real |
MSO_LOCAL_TIME |
The Mercury longitude of
the spacecraft. (Fractional Hours) |
|
23 |
ASCII Real |
MSO_LATITUDE |
The Mercury latitude of the
spacecraft. (Degrees) |
|
23 |
ASCII Real |
MSGR_MSO_X |
The X position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Y |
The Y position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Z |
The Z position of the spacecraft
in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
RAW_ENERGY |
The Energy of the particle event. (Peak – Baseline) (ADU, or Analog-to-Digital Units) |
|
23 |
ASCII Real |
ENERGY |
The calibrated energy of the particle. (keV) |
|
23 |
ASCII Real |
ENERGY_PEAK |
PHA value corresponding to the particle energy. |
|
23 |
ASCII Real |
ENERGY_BASELINE |
Baseline against which the particle energy is measured. |
|
1 |
ASCII Integer |
ION_E_FLAG |
Identifies event as either electron or ion. 0 – electron;
1 – ion. |
|
23 |
ASCII Real |
EPHEMERIS_TIME |
Solar System Barycentric event time (TDB) in the J2000 system. |
|
23 |
ASCII Real |
FRACTIONAL_YEAR |
UTC event time as a fractional year. |
|
3 |
ASCII Integer |
DAY_OF_YEAR |
Event time: Day of Year. (1-366) |
|
8 |
ASCII Integer |
INTEGRATION_TIME |
Integration/Accumulation time in seconds. (Unavailable, =0,
before FSW6) |
|
2 |
ASCII Integer |
ENERGY_BIN |
High resolution energy bin number computed by the flight
software. (0-35; Unavailable, =99, before FSW6) |
|
1 |
ASCII Integer |
MULTIPLE_HITS |
Flag indicating if more than one detector received a hit. (0
– 1) |
|
1 |
ASCII Integer |
CHANNEL_NUM |
Indicates the high energy ion or electron channel. (0-5) |
|
1 |
ASCII Integer |
PRIORITY_GROUP |
Priority group of the event (1-7) Only relevant prior to FSW6.
(after FSW6 = 99) |
|
23 |
ASCII Real |
RATE_WEIGHT |
Weight to normalize PHA events to rate channels. Only relevant prior to FSW6 (after FSW6, =
99) |
1. TIME
Spacecraft event
time (UTC) for this data record.
2. RADIAL_DIST
The distance of
the spacecraft from Mercury in the MSO frame, in units of Mercury radii..
3. MSO_LOCAL_TIME
The Mercury
longitude of the spacecraft expressed in fractional hours.
4. MSO_LATITUDE
The Mercury
latitude of the spacecraft in degrees.
5. MSGR_MSO_X
The X position of
the spacecraft in the MSO frame, in units of Mercury radii.
6. MSGR_MSO_Y
The Y position of
the spacecraft in the MSO frame, in units of Mercury radii.
7. MSGR_MSO_Z
The Z position of
the spacecraft in the MSO frame, in units of Mercury radii.
8. RAW_ENERGY
The raw PHA energy value of the event
(Peak – Baseline) in uncalibrated
Analog to Digital Units (ADUs).
9. ENERGY
Calibrated raw energy of the peak from the
Pulse Height Analysis in keVs.
10. ENERGY_PEAK
Pulse
Height Analysis (PHA) value corresponding to the particle energy in ADUs.
11. ENERGY_BASELINE
Pulse Height Analysis (PHA)
value corresponding to the baseline against which the particle energy is
measured in ADUs.
12. ION_E_FLAG
Identifies
event as either ion or electron. 0 - electron, 1 – ion.
13. EPHEMERIS_TIME
Event time in seconds since 2000 at the
Solar System Barycenter (J2000 TDB).
14. FRACTIONAL_YEAR
Event time in fractional years.
15. DAY_OF_YEAR
Day of the event.
16. INTEGRATION_TIME
Integration
time in seconds. =0 (NA) for data created prior to FSW6.
17. ENERGY_BIN
High
Resolution energy bin number computed by the flight software. =99 (NA) for data
created prior to FSW6.
18. MULTIPLE_HITS
A
flag that indicates that more than one detector received a hit. Value of 1
means multiple hits.
19. CHANNEL_NUM
Indicates
the high energy ion or electron channel (0 through 5, indicating directionality
within the 160 degree sensor field of view.
20.
PRIORITY_GROUP
Priority group of this event for PHA event collection (see instrument
description). Only used before FSW6.
21.
RATE_WEIGHT
Calculated weight to normalize this event’s significance to the particle
rate counts in the EPS_MED_CDR spectral data.
If you make a weighted histogram of these events using this weight, you
should more closely approximate the actual spectrum; i.e. this should
ameliorate the effects of the priority group sampling algorithm. Only used before FSW6.
The following are the columns as
defined by the EPS_HIRES_CDR.FMT structure file. This file defines the ASCII
table containing the EPS High Resolution Spectra data. Archive volume is
optimized by defining the table structure once and providing a reference to it
in the PDS label file. The columns are numbered according to their column order
in the table. Data_Type refers to the PDS standards data type for a particular
column in the table.
This is a new CDR created as a result of the FSW6 upload.
Table 23
EPS_HIRES_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Column Name |
Summary (see full text for column description) |
|
21 |
TIME |
TIME |
Spacecraft event time (UTC)
for this data record. |
|
8 |
ASCII Integer |
ACCUM_TIME |
Integration/Accumulation time in seconds. |
|
23 |
ASCII Real |
RADIAL_DIST |
The distance of the
spacecraft from Mercury. (Mercury radii) |
|
23 |
ASCII Real |
MSO_LOCAL_TIME |
The Mercury longitude of
the spacecraft. (Fractional Hours) |
|
23 |
ASCII Real |
MSO_LATITUDE |
The Mercury latitude of the
spacecraft. (Degrees) |
|
23 |
ASCII Real |
MSGR_MSO_X |
The X position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Y |
The Y position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Z |
The Z position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23x36 |
ASCII Real |
ION_S00_RATES |
Ion count rate spectrum for
ion direction 0, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S00_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S01_RATES |
Ion count rate spectrum for
ion direction 1, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S01_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 1, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S02_RATES |
Ion count rate spectrum for
ion direction 2, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S02_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 2, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S03_RATES |
Ion count rate spectrum for
ion direction 3, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S03_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 3, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S04_RATES |
Ion count rate spectrum for
ion direction 4, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S04_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 4, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S05_RATES |
Ion count rate spectrum for
ion direction 5, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
ION_S05_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 5, 36 energy bins. (counts/sec) |
|
23x34 |
ASCII Real |
ION_S00_FLUX |
Ion flux spectrum for ion
direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S00_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S01_FLUX |
Ion flux spectrum for ion
direction 1, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S01_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S02_FLUX |
Ion flux spectrum for ion
direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S02_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S03_FLUX |
Ion flux spectrum for ion
direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S03_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S04_FLUX |
Ion flux spectrum for ion
direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S04_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S05_FLUX |
Ion flux spectrum for ion
direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
ION_S05_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x36 |
ASCII Real |
E_S00_RATES |
Electron count rate
spectrum for ion direction 0, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S00_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 0, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S01_RATES |
Electron count rate
spectrum for ion direction 1, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S01_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 1, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S02_RATES |
Electron count rate spectrum
for ion direction 2, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S02_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 2, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S03_RATES |
Electron count rate
spectrum for ion direction 3, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S03_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 3, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S04_RATES |
Electron count rate
spectrum for ion direction 4, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S04_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 4, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S05_RATES |
Electron count rate
spectrum for ion direction 5, 36 energy bins. (counts/sec) |
|
23x36 |
ASCII Real |
E_S05_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 5, 36 energy bins. (counts/sec) |
|
23x34 |
ASCII Real |
E_S00_FLUX |
Electron flux spectrum for
ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S00_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S01_FLUX |
Electron flux spectrum for
ion direction 1, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S01_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S02_FLUX |
Electron flux spectrum for
ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S02_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S03_FLUX |
Electron flux spectrum for
ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S03_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S04_FLUX |
Electron flux spectrum for
ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S04_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S05_FLUX |
Electron flux spectrum for
ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
|
23x34 |
ASCII Real |
E_S05_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 34 energy bins. (1/cm^2 sr keV sec) |
1.
TIME
Spacecraft event time (UTC) for this data record.
2.
ACCUM_TIME
The length of the accumulation interval for this data record.
3.
RADIAL_DIST
The distance of the spacecraft from Mercury in the MSO frame, in
units of Mercury radii.
4.
MSO_LOCAL_TIME
The Mercury longitude of the spacecraft expressed in fractional
hours.
5.
MSO_LATITUDE
The Mercury latitude of the spacecraft in degrees.
6.
MSGR_MSO_X
The X position of
the spacecraft in the MSO frame, in units of Mercury radii.
7.
MSGR_MSO_Y
The Y position of
the spacecraft in the MSO frame, in units of Mercury radii.
8.
MSGR_MSO_Z
The Z position of
the spacecraft in the MSO frame, in units of Mercury radii.
9.
ION_Sn_RATES
Ion rate (counts/second) histogram for ion direction n (SSD
detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that define
the entire 160 degree field of view of the sensor for ions, and each
representing about 27 degrees out of the entire field of view. Histogram
contains the 36 bins shown in
Table 8.
10.
ION_Sn_RATES_UNC
Uncertainties for the ION_Sn_RATES.
11.
ION_Sn_FLUX
Ion flux (1/cm2 sr keV sec) histogram for ion direction
n (SSD detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that
define the entire 160 degree field of view of the sensor for ions, and each
representing about 27 degrees out of the entire field of view. Histogram
contains the 34 bins shown inTable 8 (the first and
last bins are not doubly bounded, so they do not appear in this, flux-calibrated,
spectrum).
12.
ION_Sn_FLUX_UNC
Uncertainties for the ION_Sn_FLUX,
13.
E_Sn_RATES
Electron rate (counts/second) histogram for electron direction n
(SSD detector n*2), which is 1 of the 6 electron directions (0 through 5) that
define the entire 160 degree field of view of the sensor for electrons, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 36 bins shown in
Table 9.
14.
E_Sn_RATES_UNC
Uncertainties for the COARSE_E_Sn_RATES.
15.
E_Sn_FLUX
Electron flux (1/cm2 sr keV sec) histogram for electron
direction n (SSD detector n*2), which is 1 of the 6 ion directions (0 through
5) that define the entire 160 degree field of view of the sensor for ions, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 34 bins shown in Table 9 (the first and
last bins are not doubly bounded, so they do not appear in this,
flux-calibrated, spectrum).
16.
E_Sn_FLUX_UNC
Uncertainties for the E_Sn_FLUX.
The following are the columns as
defined by the EPS_LORES_CDR.FMT structure file. This file defines the ASCII
table containing the EPS Low Resolution Spectra data. Archive volume is
optimized by defining the table structure once and providing a reference to it
in the PDS label file. The columns are numbered according to their column order
in the table. Data_Type refers to the PDS standards data type for a particular
column in the table.
This is a new CDR created as a result of the FSW6 upload.
Table 24 EPS_LORES_CDR.FMT Columns
|
Length(bytes) |
Data Type |
Column Name |
Summary (see full text for column description) |
|
21 |
TIME |
TIME |
Spacecraft event time (UTC)
for this data record. |
|
8 |
ASCII Integer |
ACCUM_TIME |
Integration/Accumulation
time in seconds. |
|
23 |
ASCII Real |
RADIAL_DIST |
The distance of the
spacecraft from Mercury. (Mercury radii) |
|
23 |
ASCII Real |
MSO_LOCAL_TIME |
The Mercury longitude of
the spacecraft. (Fractional Hours) |
|
23 |
ASCII Real |
MSO_LATITUDE |
The Mercury latitude of the
spacecraft. (Degrees) |
|
23 |
ASCII Real |
MSGR_MSO_X |
The X position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Y |
The Y position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII Real |
MSGR_MSO_Z |
The Z position of the
spacecraft in the MSO frame. (Mercury radii) |
|
23x12 |
ASCII Real |
ION_S00_RATES |
Ion count rate spectrum for
ion direction 0, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S00_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 0, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S01_RATES |
Ion count rate spectrum for
ion direction 1, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S01_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 1, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S02_RATES |
Ion count rate spectrum for
ion direction 2, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S02_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 2, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S03_RATES |
Ion count rate spectrum for
ion direction 3, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S03_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 3, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S04_RATES |
Ion count rate spectrum for
ion direction 4, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S04_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 4, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S05_RATES |
Ion count rate spectrum for
ion direction 5, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
ION_S05_RATES_UNC |
Ion count rate spectrum
uncertainty for ion direction 5, 12 energy bins. (counts/sec) |
|
23x10 |
ASCII Real |
ION_S00_FLUX |
Ion flux spectrum for ion
direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S00_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S01_FLUX |
Ion flux spectrum for ion
direction 1, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S01_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S02_FLUX |
Ion flux spectrum for ion
direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S02_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S03_FLUX |
Ion flux spectrum for ion
direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S03_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S04_FLUX |
Ion flux spectrum for ion
direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S04_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S05_FLUX |
Ion flux spectrum for ion
direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
ION_S05_FLUX_UNC |
Ion flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII Real |
E_S00_RATES |
Electron count rate
spectrum for ion direction 0, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S00_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 0, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S01_RATES |
Electron count rate
spectrum for ion direction 1, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S01_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 1, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S02_RATES |
Electron count rate
spectrum for ion direction 2, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S02_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 2, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S03_RATES |
Electron count rate
spectrum for ion direction 3, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S03_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 3, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S04_RATES |
Electron count rate
spectrum for ion direction 4, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S04_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 4, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S05_RATES |
Electron count rate
spectrum for ion direction 5, 12 energy bins. (counts/sec) |
|
23x12 |
ASCII Real |
E_S05_RATES_UNC |
Electron count rate
spectrum uncertainty for ion direction 5, 12 energy bins. (counts/sec) |
|
23x10 |
ASCII Real |
E_S00_FLUX |
Electron flux spectrum for
ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S00_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S01_FLUX |
Electron flux spectrum for
ion direction 1, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S01_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S02_FLUX |
Electron flux spectrum for
ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S02_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S03_FLUX |
Electron flux spectrum for
ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S03_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S04_FLUX |
Electron flux spectrum for
ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S04_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S05_FLUX |
Electron flux spectrum for
ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x10 |
ASCII Real |
E_S05_FLUX_UNC |
Electron flux spectrum
uncertainty for ion direction 0, 10 energy bins. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII Real |
FAST_ENERGY_RATE |
The 12 fast energy hardware
count rates. (counts/sec) |
|
23x12 |
ASCII Real |
SHAPED_ENERGY_RATE |
The 12 shaped energy
hardware count rates. (counts/sec) |
|
23 |
ASCII Real |
ION_EVENT_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
E_EVENT_RATE |
Electron event hardware
count rate. (counts/sec) |
|
23 |
ASCII Real |
ION_PROCESSED_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
E_PROCESSED_RATE |
Ion event hardware count
rate. (counts/sec) |
|
23 |
ASCII Real |
PILEUP_ION_RATE |
Rate of ion events
discarded due to pileup condition. (counts/sec) |
|
23 |
ASCII Real |
PILEUP_E_RATE |
Rate of electron events
discarded due to pileup condition. (counts/sec) |
|
23 |
ASCII Real |
REJECTED_ION_RATE |
Rate of ion events rejected
due to negative energy. (counts/sec) |
|
23 |
ASCII Real |
REJECTED_E_RATE |
Rate of electron events
rejected due to negative energy. (counts/sec) |
|
23 |
ASCII Real |
MULTIPLE_HITS_RATE |
Rate of events discarded
due to multiple hits. (counts/sec) |
Spacecraft event time (UTC) for this data record.
2.
ACCUM_TIME
The length of the accumulation interval for this data record.
3.
RADIAL_DIST
The distance of the spacecraft from Mercury in the MSO frame, in
units of Mercury radii..
4.
MSO_LOCAL_TIME
The Mercury longitude of the spacecraft expressed in fractional
hours.
5.
MSO_LATITUDE
The Mercury latitude of the spacecraft in degrees.
The X position of
the spacecraft in the MSO frame, in units of Mercury radii.
The Y position of
the spacecraft in the MSO frame, in units of Mercury radii.
The Z position of
the spacecraft in the MSO frame, in units of Mercury radii.
Ion rate (counts/second) histogram for ion direction n (SSD
detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that define
the entire 160 degree field of view of the sensor for ions, and each
representing about 27 degrees out of the entire field of view. Histogram
contains the 12 bins shown in
Table 10.
10.
ION_Sn_RATES_UNC
Uncertainties for the ION_Sn_RATES.
11.
ION_Sn_FLUX
Ion flux (1/cm2 sr keV sec) histogram for ion direction
n (SSD detector n*2+1), which is 1 of the 6 ion directions (0 through 5) that
define the entire 160 degree field of view of the sensor for ions, and each representing
about 27 degrees out of the entire field of view. Histogram contains the 10
bins shown in Table 10 (the first and
last bins are not doubly bounded, so they do not appear in this,
flux-calibrated, spectrum).
12.ION_Sn_FLUX_UNC
Uncertainties for the ION_Sn_FLUX.
13.E_Sn_RATES
Electron rate (counts/second) histogram for electron direction n
(SSD detector n*2), which is 1 of the 6 electron directions (0 through 5) that
define the entire 160 degree field of view of the sensor for electrons, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 12 bins shown in Table 11.
14.E_Sn_RATES_UNC
Uncertainties for the COARSE_E_Sn_RATES.
15.E_Sn_FLUX
Electron flux (1/cm2 sr keV sec) histogram for electron
direction n (SSD detector n*2), which is 1 of the 6 ion directions (0 through
5) that define the entire 160 degree field of view of the sensor for ions, and
each representing about 27 degrees out of the entire field of view. Histogram
contains the 10 bins shown in
Table 11 (the first and last bins are not doubly
bounded, so they do not appear in this, flux-calibrated, spectrum).
16.E_Sn_FLUX_UNC
Uncertainties for the E_Sn_FLUX.
17.
FAST_ENERGY_RATE
Counts the firing rate of a discriminator
when an analog signal exceeds a settable threshold. The discriminator is
connected to the output of the pole-zero shaping circuit. There are 12 values,
one for each SSD.
18.
SHAPED_ENERGY_RATE
Counts the firing of a discriminator when
an analog signal exceeds a settable threshold. The discriminator is connected
to the output of the 3 pole Gaussian shaping circuit. There are 12 values, one
for each SSD.
19.
ION_EVENT_RATE
Hardware rate (counts/sec) for all classified Ion events
registered in the fast processing electronics upstream from the Event
Processing Computer. Because the Event Processing Computer can process at most
about 5000 events, this counter allows the user to renormalize the processed
output rates to retrieve true intensities.
20.
E_EVENT_RATE
Hardware rate
(counts/sec) for all classified Electron events registered in the fast
processing electronics upstream from the Event Processing Computer. Because the
Event Processing Computer can process at most about 5000 events, this counter
allows the user to renormalize the processed output rates to retrieve true
intensities.
21.
ION_PROCESSED_RATE
Rate of ion
events processed by the Event Processing Computer during the accumulation interval
22.
E_PROCESSED_RATE
Rate
(counts/sec) of electron events processed by the Event Processing Computer
during the accumulation interval.
23.
PILEUP_ION_RATE
Rate of ion events discarded
by the Event Processing Computer due to pileup condition.
24.
PILEUP_E_RATE
Rate
of electron events discarded by the Event Processing Computer due to pileup
condition.
25.
REJECTED_ION_RATE
Rate of ions rejected due to negative
energy.
26.
REJECTED_E_RATE
Rate of electrons rejected due to negative
energy.
27.
MULTIPLE_HIT_RATE
Ion or electron events
rejected due to multiple hits.
The columns defined by the EPS_SUM_CDR.FMT structure file are identical to those defined by the EPS_LORES_CDR.FMT file. The EPS Summary data contains the same data columns as EPS LoRes data, but sampled at the (lower) EPS HiRes rate. This serves the dual purpose of facilitating comparisons between HiRes and LoRes data and providing a low bandwidth data type which can be used for quick look verification during spacecraft operations. Refer to Section 8.5 for a description of the EPS_SUM_CDR.FMT columns.
This is a new CDR created as a result of the FSW6 upload.
New in FSW6 is the Scan data. In scan mode, EPS varies the energy
thresholds integrating hardware rates at each threshold setting (defined in
tables). The thresholds are changed
three times, then the base thresholds are restored. A scan is defined as four threshold settings:
three offsets and one nominal. At each threshold step, a subset of the hardware
rate counters are accumulated for 1⁄4 second. The Scan mode gives EPS the ability to lower
its electronics threshold by temporary suspending the processor operation.
Scan rates are reported in two
forms. Simple rates or fluxes represent
the counts (or calibrated flux) above the threshold values as shown in Table
12
and Table
13.
Delta rates or fluxes represent the counts (or
calibrated flux) obtained by subtracting counts in “adjacent” scans so that the
resulting value mimics a double bounded energy bin.
Table 25 EPS_SCAN_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
|
21 |
TIME |
TIME |
Spacecraft
event time (UTC) for this data record. |
|
8 |
ASCII
Integer |
ACCUM_TIME |
Integration/Accumulation
time in seconds. |
|
23 |
ASCII
Real |
RADIAL_DIST |
The
distance of the spacecraft from Mercury. (Mercury radii) |
|
23 |
ASCII
Real |
MSO_LOCAL_TIME |
The
Mercury longitude of the spacecraft. (Fractional Hours) |
|
23 |
ASCII
Real |
MSO_LATITUDE |
The
Mercury latitude of the spacecraft. (Degrees) |
|
23 |
ASCII
Real |
MSGR_MSO_X |
The
X position of the spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII
Real |
MSGR_MSO_Y |
The
Y position of the spacecraft in the MSO frame. (Mercury radii) |
|
23 |
ASCII
Real |
MSGR_MSO_Z |
The
Z position of the spacecraft in the MSO frame. (Mercury radii) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_OFFSET_A |
Fast-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_UNC_OFFSET_A |
Fast-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_OFFSET_A |
Fast-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_UNC_OFFSET_A |
Fast-mode
delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_OFFSET_A |
Shaped-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_UNC_OFFSET_A |
Shaped-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_OFFSET_A |
Shaped-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_UNC_OFFSET_A |
Shaped
-mode delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_OFFSET_A |
Fast-mode
count delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_UNC_OFFSET_A |
Fast-mode
count delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_OFFSET_A |
Fast-mode
count scan rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_UNC_OFFSET_A |
Fast-mode
count scan rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_OFFSET_B |
Fast-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_UNC_OFFSET_B |
Fast-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_OFFSET_B |
Fast-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_UNC_OFFSET_B |
Fast-mode
delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_OFFSET_B |
Shaped-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_UNC_OFFSET_B |
Shaped-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_OFFSET_B |
Shaped-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_UNC_OFFSET_B |
Shaped
-mode delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_OFFSET_B |
Fast-mode
count delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_UNC_OFFSET_B |
Fast-mode
count delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_OFFSET_B |
Fast-mode
count scan rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_UNC_OFFSET_B |
Fast-mode
count scan rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_OFFSET_C |
Fast-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_UNC_OFFSET_C |
Fast-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_OFFSET_C |
Fast-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_UNC_OFFSET_C |
Fast-mode
delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_OFFSET_C |
Shaped-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_UNC_OFFSET_C |
Shaped-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_OFFSET_C |
Shaped-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_UNC_OFFSET_C |
Shaped
-mode delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_OFFSET_C |
Fast-mode
count delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_UNC_OFFSET_C |
Fast-mode
count delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_OFFSET_C |
Fast-mode
count scan rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_UNC_OFFSET_C |
Fast-mode
count scan rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_OFFSET_D |
Fast-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_RATES_UNC_OFFSET_D |
Fast-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_OFFSET_D |
Fast-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_DELTA_FLUXES_UNC_OFFSET_D |
Fast-mode
delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_OFFSET_D |
Shaped-mode
delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_RATES_UNC_OFFSET_D |
Shaped-mode
delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_OFFSET_D |
Shaped-mode
delta flux. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
SHAPED_DELTA_FLUXES_UNC_OFFSET_D |
Shaped
-mode delta flux uncertainty. One for each SSD. (1/cm^2 sr keV sec) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_OFFSET_D |
Fast-mode
count delta rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
FAST_SCAN_RATES_UNC_OFFSET_D |
Fast-mode
count delta rate uncertainty. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_OFFSET_D |
Fast-mode
count scan rate. One for each SSD. (counts/second) |
|
23x12 |
ASCII
Real |
SHAPED_SCAN_RATES_UNC_OFFSET_D |
Fast-mode
count scan rate uncertainty. One for each SSD. (counts/second) |
Spacecraft event
time (UTC) for this data record.
2. ACCUM_TIME
The length of the
accumulation interval for this data record.
3. RADIAL_DIST
The distance of
the spacecraft from Mercury in the MSO frame, in units of Mercury radii..
4. MSO_LOCAL_TIME
The Mercury
longitude of the spacecraft expressed in fractional hours.
5. MSO_LATITUDE
The Mercury
latitude of the spacecraft in degrees.
The X position of
the spacecraft in the MSO frame, in units of Mercury radii.
7.
MSGR_MSO_Y
The Y position of
the spacecraft in the MSO frame, in units of Mercury radii.
8.
MSGR_MSO_Z
The Z position of
the spacecraft in the MSO frame, in units of Mercury radii.
9. FAST_DELTA_RATES_OFFSET_n
Count rate of the
firing of a discriminator when an analog signal exceeds a settable threshold,
for offset n threshold, where n is one of A, B, C, or D. The discriminator is
connected to the output of the pole-zero shaping circuit. Reported as a “delta”
value.
10.FAST_DELTA_RATES_UNC_OFFSET_n
Uncertainties for the FAST_DELTA_RATES, for offset n threshold, where n is one of A, B,
C, or D.
11.FAST_DELTA_FLUXES_OFFSET_n
Calibrated flux
of the delta value of the firing rate of a discriminator when an analog signal
exceeds a settable threshold, for offset n threshold, where n is one of A, B,
C, or D. The discriminator is connected to the output of the pole-zero shaping
circuit.
Uncertainties for the FAST_DELTA_FLUXES, for offset n threshold, where n is one of A, B,
C, or D.
Count rate of the
firing of a discriminator when an analog signal exceeds a settable threshold,
for offset n threshold, where n is one of A, B, C, or D. The discriminator is
connected to the output of the 3 pole Gaussian shaping circuit. Reported as a
“delta” value.
Uncertainties for the SHAPED_DELTA_RATES.
Calibrated flux
of the delta value of the firing rate of a discriminator when an analog signal
exceeds a settable threshold, for offset n threshold, where n is one of A, B,
C, or D. The discriminator is connected to the output of the 3 pole Gaussian
shaping circuit.
Uncertainties for the SHAPED_DELTA_FLUXES, for offset n threshold, where n is one of A,
B, C, or D.
Count rate of the
firing of a discriminator when an analog signal exceeds a settable threshold,
for offset n threshold, where n is one of A, B, C, or D. The discriminator is
connected to the output of the pole-zero shaping circuit.
Uncertainties for the FAST_SCAN_RATES, for offset n threshold, where n is one of A, B,
C, or D.
Count rate of the
firing of a discriminator when an analog signal exceeds a settable threshold,
for offset n threshold, where n is one of A, B, C, or D. The discriminator is
connected to the output of the 3 pole Gaussian shaping circuit.
Uncertainties for the SHAPED_SCAN_RATES, for offset n threshold, where n is one of A,
B, C, or D.
The following are the columns as
defined by the FIPS_HI_CDR.FMT structure file. This file defines the ASCII
table containing the FIPS High Priority data. Archive volume is optimized by
defining the table structure once and providing a reference to it in the PDS
label file. The columns are numbered according to their column order in the
table. Data_Type refers to the PDS standards data type for a particular column
in the table.
A FIPS flight software upload was implemented on
9/6/2007. The FIPS_SCANTYPE and STOP_DIFFINTENS columns were introduced as a
result. The values for these columns are not meant to be valid prior to
9/6/2007.
Table 26
FIPS_HI_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
|
16 |
ASCII Real |
MET |
Mission Elapsed Time in seconds. |
|
21 |
TIME |
TIME |
UTC time string. |
|
7 |
ASCII Integer |
DATA_QUALITY |
Data quality flag. |
|
4 |
ASCII Integer |
FIPS_SCANTYPE |
Indicates FIPS Scan mode. |
|
10 X 64 |
ASCII Real |
PROTON_V_DIST0 |
64 element array of normalized proton velocity distribution
values. |
|
10 X 64 |
ASCII Real |
START_DIFFINTENS |
64 element array of start particle differential intensity. |
|
10 X 64 |
ASCII Real |
STOP_DIFFINTENS |
64 element array of stop particle differential intensity. |
|
10 X 64 |
ASCII Real |
VALID_EVT_DIFFINTENS |
64 element array of valid event particle differential intensity. |
|
10 X 64 |
ASCII Real |
PROTON_DIFFINTENS |
64 element array of proton particle differential intensity. |
|
10 X 64 |
ASCII Real |
EVT_PROC_DIFFINTENS |
64 element array of event processed particle differential
intensity. |
Mission elapsed time in seconds at the end of the accumulation.
Spacecraft event time (UTC)
for this data record.
Data quality flag, taking on values of 0 (bad)
and 1 (good).
Indicates the FIPS Scan Mode. Tables referenced
here are one of the eight E/q stepping tables loaded into the instrument. See
the EPPS CDR SIS in the EPPS Document Archive Volume for details. =0 Normal Scan, =1 High Temp Scan, =2 Burst
Scan, =3 Test Scan, =4 Table 4, =5 Table 5, =6 Table 6, =7 Table 7.
A 64-element normalized proton velocity distribution function based on the proton events detected during the first 64-step voltage scan of each 10-scan sequence.
The start particle differential intensity, in counts per (keV/e) per sec per cm**2 per sr. Sampled at each of the 64 steps in the 1st scan of a 10-scan sequence.
The stop particle differential intensity, in counts per (keV/e) per sec per cm**2 per sr. Sampled at each of the 64 steps in the 1st scan of a 10-scan sequence.
The valid event particle differential intensity, in counts per (keV/e) per sec per cm**2 per sr. Sampled at each of the 64 steps in the 1st scan of a 10-scan sequence.
The proton particle differential intensity, in counts per (keV/e) per sec per cm**2 per sr. Sampled at each of the 64 steps in scan 10 of a 10-scan sequence.
The events processed particle differential intensity, in counts per (keV/e) per sec per cm**2 per sr. Sampled at each of the 64 steps in scan 10 of a 10-scan sequence.
The following are the columns as
defined by the FIPS_MED_CDR.FMT structure file. This file defines the ASCII
table containing the FIPS Medium Priority spectra data. Archive volume is
optimized by defining the table structure once and providing a reference to it
in the PDS label file. The columns are numbered according to their column order
in the table. Data_Type refers to the PDS standards data type for a particular
column in the table.
A FIPS flight software upload was implemented on
9/6/2007. The FIPS_SCANTYPE and STOP_DIFFINTENS columns were introduced as a
result. The values for these columns are not meant to be valid prior to
9/6/2007.
The FSW6 upload was done on 8/18/2008 and implemented on
8/19/2008. The software update retired the FIPS Medium
Priority Spectra packet. Thus there are no FIPS Medium
Priority CDRs on or after 8/19/2008.
Table 27
FIPS_MED_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
|
16 |
ASCII Real |
MET |
Mission Elapsed Time in seconds. |
|
21 |
TIME |
TIME |
UTC time string. |
|
7 |
ASCII Integer |
DATA_QUALITY |
Data quality flag. |
|
4 |
ASCII Integer |
FIPS_SCANTYPE |
Indicates FIPS Scan mode. |
|
10 X 64 |
ASCII Real |
PROTON_V_DIST210 |
64 element array of Normalized proton velocity distribution
values. |
|
10 X 64 |
ASCII Real |
START_DIFFINTENS |
64 element array of start differential intensity. |
|
10 X 64 |
ASCII Real |
STOP_DIFFINTENS |
64 element array of stop differential intensity. |
|
10 X 64 |
ASCII Real |
VALID_EVT_DIFFINTENS |
64 element array of valid event differential intensity. |
|
10 X 64 |
ASCII Real |
PROTON_DIFFINTENS |
64 element array of proton differential intensity. |
|
10 X 64 |
ASCII Real |
EVT_PROC_DIFFINTENS |
64 element array of events processed differential intensity. |
Mission elapsed time in seconds at the end of the accumulation.
Spacecraft event time (UTC)
for this data record.
Data quality flag, taking on values of 0 (bad)
and 1 (good).
Indicates the FIPS Scan Mode. Tables referenced
here are one of the eight E/q stepping tables loaded into the instrument. See
the EPPS CDR SIS in the EPPS Document Archive Volume for details. =0 Normal Scan, =1 High Temp Scan, =2 Burst
Scan, =3 Test Scan, =4 Table 4, =5 Table 5, =6 Table 6, =7 Table 7.
A 64-element normalized proton velocity distribution accumulated over each of scans 2-10 in the 10 scan sequence, expressed as a unit-less probability..
Start differential intensity, in counts per (keV/e) per sec per cm**2 per sr.
Stop differential intensity, in counts per (keV/e) per sec per cm**2 per sr.
Valid event differential intensity, in counts per (keV/e) per sec per cm**2 per sr.
Proton differential intensity, in counts per (keV/e) per sec per cm**2 per sr.
Events processed differential intensity, in counts per (keV/e) per sec per cm**2 per sr.
The following are the columns as
defined by the FIPS_PHA_CDR.FMT structure file. This file defines the ASCII
table containing the FIPS Pulse Height Analysis (PHA) event data. Archive
volume is optimized by defining the table structure once and providing a
reference to it in the PDS label file. The columns are numbered according to
their column order in the table. Data_Type refers to the PDS standards data
type for a particular column in the table.
A FIPS flight software upload was implemented on
9/6/2007. The FIPS_SCANTYPE column was introduced as a result. The value for this
column is not meant to be valid prior to 9/6/2007.
In addition, another flight software upload
(FSW7) was done on 8/18/2009. As a result, the PRIORITY_DECIMATION column
meaning is different before FSW7. See the description for details.
Table 28
FIPS_PHA_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
|
16 |
ASCII Real |
MET |
Mission Elapsed Time in seconds. |
|
21 |
TIME |
TIME |
UTC time string. |
|
8 |
ASCII Integer |
DATA_QUALITY |
Data quality flag. |
|
8 |
ASCII Integer |
FIPS_SCANTYPE |
Indicates FIPS Scan mode. |
|
7 |
ASCII Integer |
PRIORITY_DECIMATION |
PHA priority ID (pre-FSW7); proton hardware decimation level
(post-FSW7). |
|
4 |
ASCII Integer |
STEP_NUM |
E/q step number. |
|
6 |
ASCII Real |
ENERGY_PER_CHARGE |
E/q value. |
|
4 |
ASCII Integer |
X |
Calculated value for FIPS event. |
|
4 |
ASCII Integer |
Y |
Calculated value for FIPS event. |
|
7 |
ASCII Real |
ZENITH_ANGLE |
Incident zenith angle for particle. |
|
7 |
ASCII Real |
AZIMUTHAL_ANGLE |
Incident azimuthal angle for particle. |
|
5 |
ASCII Integer |
TIME_OF_FLIGHT |
Time of flight. |
|
5 |
ASCII Integer |
TIME_OF_FLIGHT_NS |
Time of flight in nanoseconds. |
|
6 |
ASCII Integer |
WEDGE |
Wedge number. |
|
6 |
ASCII Integer |
STRIP |
Strip number. |
|
6 |
ASCII Integer |
ZIGZAG |
Zigzag number. |
|
10 |
ASCII Real |
MASS_PER_CHARGE |
Estimated mass per charge for particle. |
|
10 |
ASCII Real |
WEIGHT |
Weight for particle. |
Mission elapsed time in seconds at the end of the accumulation.
Spacecraft event time (UTC)
for this data record.
Data quality flag, taking on values of 0 (bad)
and 1 (good).
Indicates the FIPS Scan Mode and particle type. Tables
referenced here are one of the eight E/q stepping tables loaded into the
instrument. See the EPPS CDR SIS for details. =0 Normal Scan Heavy Ion, =1 High
Temp Scan Heavy Ion, =2 Burst Scan Heavy Ion, =3 Test Scan Heavy Ion, =4 Table
4 Heavy Ion, =5 Table 5 Heavy Ion, =6 Table 6 Heavy Ion, =7 Table 7 Heavy Ion,
=8 Normal Scan Proton, =9 High Temp Scan Proton, =10 Burst Scan Proton, =11
Test Scan Proton, =12 Table 4 Proton, =13 Table 5 Proton, =14 Table 6 Proton,
=15 Table 7 Proton.
Prior to FSW7 this column records the priority
level of the PHA data. 0 = High Priority, 1 = Medium priority, 2 = Low
priority. After FSW7 this column records the proton hardware decimation level
for
proton PHAs or =99 for Heavy Ion PHAs.
E/q Step Number (0-63) at which particle was measured.
E/q value in keV/e corresponding to step number at which particle was measured.
In FSW4, FSW5, and FSW7, X is computed as
[128*(w+(w-z)/5)/sum],
and in FSW6, X is computed as
[ 96*(s+(s-z)/5)/sum]
where
w
= wedge - wedge_offset
s
= strip - strip_offset
z
= 14*(zigzag - zigzag_offset)/10
sum = w+s+z.
A value of -9999 means X is
N/A.
In FSW4, FSW5, and FSW7, Y is computed as
[128*(s+(s-z)/5)/sum],
and in FSW6, Y is computed as
[100*(s+2*(s-z)/11)/sum]
where
w
= wedge - wedge_offset
s
= strip - strip_offset
z
= 14*(zigzag-zigzag_offset)/10
sum = w+s+z.
A value of -9999 means Y is N/A.
Incident zenith angle for particle in degrees.
Incident azimuthal angle
for particle in degrees.
Time of flight in digital channels.
Time of flight in nanoseconds.
Wedge number. A value of
-9999 means WEDGE is N/A.
Strip number. A value of -9999 means STRIP is N/A.
Zigzag number. A value of -9999 means ZIGZAG is N/A.
Estimated mass per charge (m/q) for particle.
Weight for particle, includes instrument-related factors such as efficiency and angle dependence.
The following are the columns as
defined by the FIPS_SCAN_CDR.FMT structure file. This file defines the ASCII
table containing the FIPS Scan data. Archive volume is optimized by defining
the table structure once and providing a reference to it in the PDS label file.
The columns are numbered according to their column order in the table.
Data_Type refers to the PDS standards data type for a particular column in the
table.
Available only after the FSW6 upload..
Table 29
FIPS_SCAN_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
|
16 |
ASCII Real |
MET |
Mission Elapsed Time in seconds. |
|
21 |
TIME |
TIME |
UTC time string. |
|
7 |
ASCII Integer |
DATA_QUALITY |
Data quality flag. |
|
4 |
ASCII Integer |
FIPS_SCANTYPE |
Indicates FIPS Scan mode. |
|
10 X 64 |
ASCII Real |
START_DIFFINTENS |
Start differential intensity. |
|
10 X 64 |
ASCII Real |
STOP_DIFFINTENS |
Stop differential intensity. |
|
10 X 64 |
ASCII Real |
VALID_EVT_DIFFINTENS |
Valid event differential intensity. |
|
10 X 64 |
ASCII Real |
PROTON_DIFFINTENS |
Proton differential intensity. |
|
10 X 64 |
ASCII Real |
EVT_PROC_DIFFINTENS |
Events processed differential intensity. |
Mission elapsed time in seconds at the end of the accumulation.
Spacecraft event time (UTC)
for this data record.
Data quality flag, taking on values of 0 (bad)
and 1 (good).
Indicates the FIPS Scan Mode. Tables referenced
here are one of the eight E/q stepping tables loaded into the instrument. See
the EPPS CDR SIS in the EPPS Document Archive Volume for details. =0 Normal Scan, =1 High Temp Scan, =2 Burst
Scan, =3 Test Scan, =4 Table 4, =5 Table 5, =6 Table 6, =7 Table 7.
5.
START_DIFFINTENS
Start differential
intensity sampled at each E/q step in the scan,
in counts per (keV/e) per
sec per cm**2 per sr.
6.
STOP_DIFFINTENS
Stop differential
intensity sampled at each E/q step in the scan, in counts per (keV/e) per sec per cm**2 per sr.
7.
VALID_EVT_DIFFINTENS
Valid
event differential
intensity sampled at each E/q step in the scan, in counts per (keV/e) per sec per cm**2 per sr.
8. PROTON_DIFFINTENS
Proton
rate counter differential
intensity sampled at each E/q step in the scan, in counts per (keV/e) per sec per cm**2 per sr.
9.
EVT_PROC_DIFFINTENS
Events processed differential
intensity sampled at each E/q step in the scan, in counts per (keV/e) per sec per cm**2 per sr.
The following are the columns as
defined by the FIPS_HRPVD_CDR.FMT structure file. This file defines the ASCII
table containing the Hi-resolution normalized proton velocity distributions.
Archive volume is optimized by defining the table structure once and providing
a reference to it in the PDS label file. The columns are numbered according to
their column order in the table. Data_Type refers to the PDS standards data
type for a particular column in the table.
Available only after the FSW6 upload.
Table 30
FIPS_HRPVD_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
||
|
16 |
ASCII Real |
MET |
Mission Elapsed Time in seconds. |
||
|
21 |
TIME |
TIME |
UTC time string. |
||
|
7 |
ASCII Integer |
DATA_QUALITY |
Data quality flag. |
||
|
4 |
ASCII Integer |
FIPS_SCANTYPE |
Indicates FIPS Scan mode. |
||
|
11 X 32 |
ASCII Real |
PROTONV_L00 |
Line 0 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L01 |
Line 1 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L02 |
Line 2 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L03 |
Line 3 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L04 |
Line 4 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L05 |
Line 5 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L06 |
Line 6 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L07 |
Line 7 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L08 |
Line 8 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L09 |
Line 9 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L10 |
Line 10 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L11 |
Line 11 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L12 |
Line 12 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L13 |
Line 13 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L14 |
Line 14 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L15 |
Line 15 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L16 |
Line 16 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L17 |
Line 17 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L18 |
Line 18 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L19 |
Line 19 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L20 |
Line 20 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L21 |
Line 21 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L22 |
Line 22 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L23 |
Line 23 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L24 |
Line 24 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L25 |
Line 25 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L26 |
Line 26 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L27 |
Line 27 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L28 |
Line 28 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L29 |
Line 29 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L30 |
Line 30 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
11 X 32 |
ASCII Real |
PROTONV_L31 |
Line 31 of a 32X32 hi-res proton vel distribution, integrated
over 10 scan seq |
||
|
10 |
ASCII Real |
PROTON_L |
Probability of protons in
left edge of the 32X32 window. |
||
|
10 |
ASCII Real |
PROTON_R |
Probability of protons in
right edge of the 32X32 window. |
||
|
10 |
ASCII Real |
PROTON_BOT |
Probability of protons in
bottom edge of the 32X32 window. |
||
|
10 |
ASCII Real |
PROTON_TOP |
Probability of protons in
top edge of the 32X32 window. |
||
Mission elapsed time in seconds at the end of the accumulation.
Spacecraft event time (UTC)
for this data record.
Data quality flag, taking on values of 0 (bad)
and 1 (good).
Indicates the FIPS Scan Mode. Tables referenced
here are one of the eight E/q stepping tables loaded into the instrument. See
the EPPS CDR SIS in the EPPS Document Archive Volume for details. =0 Normal Scan, =1 High Temp Scan, =2 Burst
Scan, =3 Test Scan, =4 Table 4, =5 Table 5, =6 Table 6, =7 Table 7.
5.
PROTONV_L00
Line 0 of a
32x32 high-resolution normalized proton velocity distribution, integrated over
a 10-scan sequence, expressed as a unit-less probability..
6.
PROTONV_L01
Line
1 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
7.
PROTONV_L02
Line
2 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
8.
PROTONV_L03
Line
3 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
9.
PROTONV_L04
Line
4 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
10.
PROTONV_L05
Line
5 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
11.
PROTONV_L06
Line
6 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
12.
PROTONV_L07
Line
7 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
13.
PROTONV_L08
Line
8 of a 32x32 high-resolution normalized proton velocity distribution, integrated
over a 10-scan sequence, expressed as a unit-less probability..
14.
PROTONV_L09
Line
9 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
15.
PROTONV_L10
Line
10 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
16.
PROTONV_L11
Line
11 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
17.
PROTONV_L12
Line
12 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
18.
PROTONV_L13
Line
13 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
19.
PROTONV_L14
Line
14 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
20.
PROTONV_L15
Line
15 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
21.
PROTONV_L16
Line
16 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
22.
PROTONV_L17
Line
17 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
23.
PROTONV_L18
Line
18 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
24.
PROTONV_L19
Line
19 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
25.
PROTONV_L20
Line
20 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
26.
PROTONV_L21
Line
21 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
27.
PROTONV_L22
Line
22 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
28.
PROTONV_L23
Line
23 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
29.
PROTONV_L24
Line
24 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
30.
PROTONV_L25
Line
25 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
31.
PROTONV_L26
Line
26 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
32.
PROTONV_L27
Line
27 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
33.
PROTONV_L28
Line
28 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
34.
PROTONV_L29
Line
29 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
35.
PROTONV_L30
Line
30 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
36.
PROTONV_L31
Line
31 of a 32x32 high-resolution normalized proton velocity distribution,
integrated over a 10-scan sequence, expressed as a unit-less probability..
37.
PROTON_L
Probability
of protons off the left edge of the 32x32 window.
38.
PROTON_R
Probabilty
of protons off the right edge of the 32x32 window.
39.
PROTON_BOT
Probability
of protons off the bottom edge of the 32x32 window.
40.
PROTON_TOP
Probabilty
of protons off the top edge of the 32x32 window.
The following are the columns as
defined by the FIPS_EQ.FMT structure file. This file defines the ASCII table
containing the FIPS energy per charge ancillary data. Archive volume is
optimized by defining the table structure once and providing a reference to it
in the PDS label file. The columns are numbered according to their column order
in the table. Data_Type refers to the PDS standards data type for a particular
column in the table.
Table 31
FIPS_SCAN_CDR.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column description) |
|
6 |
ASCII Integer |
STEP |
Position in electrostatic analyzer voltage stepping sequence. |
|
6 |
ASCII Real |
EQ_TABLE_0 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_0 |
Index of E/q value in flight software DSHV Index Table, the table of possible DSHV (E/q) values that can be specified in a given stepping table. Useful for grouping E/q values in natural bins. Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_0 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_0 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_1 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_1 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for
grouping E/q values in natural bins.
Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_1 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_1 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_2 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_2 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for grouping
E/q values in natural bins. Range
0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_2 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_2 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_3 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_3 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for
grouping E/q values in natural bins.
Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_3 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_3 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_4 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_4 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for
grouping E/q values in natural bins.
Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_4 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_4 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_5 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_5 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for
grouping E/q values in natural bins.
Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_5 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_5 |
Proton threshold in nanoseconds. Events with TOF < threshold are
classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_6 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_6 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for
grouping E/q values in natural bins.
Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_6 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_6 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
|
6 |
ASCII Real |
EQ_TABLE_7 |
E/q in keV/e of measurement. |
|
6 |
ASCII Integer |
DSHV_TABLE_7 |
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a
given stepping table. Useful for
grouping E/q values in natural bins.
Range 0..63. |
|
7 |
ASCII Integer |
ACCUM_TIME_7 |
Accumulation time for measurement in milliseconds. |
|
9 |
ASCII Real |
H_THRESH_TABLE_7 |
Proton threshold in
nanoseconds. Events with TOF <
threshold are classified as protons, and treated differently than heavy ions. |
Position in electrostatic analyzer voltage stepping sequence.
E/q in keV/e of measurement.
Index of E/q
value in flight software DSHV Index
Table, the table of possible DSHV (E/q) values that can be specified in a given
stepping table. Useful for grouping E/q
values in natural bins. Range 0..63.
Accumulation time for
measurement in milliseconds.
5.
H_THRESH_TABLE_n
Start flux
sampled at each E/q step in the scan, in counts per (keV/e) per sec per cm**2
per sr.
The following are the columns as defined by the FIPS_FOV Pixel_CDR.FMT structure file. This file defines the ASCII table containing the FIPS FOV Pixel normalizations. The archive volume is optimized by defining the table structure once and providing a reference to it in the PDS label file. The columns are numbered according to their column order in the table. Data Type refers to the PDS standards data type for a particular column in the table.
The INDEX field values are unique for a given day and may be used to match data in this file to that in the two FIPS CDR files for the same day. This fact is used to avoid data duplication: Universal Time (UTC) and MESSENGER positions are given only this file.
Table 32 FIPS_FOVPIXEL.FMT Columns
|
Length (bytes) |
Data Type |
Field Name |
Summary (see full text for column
description) |
|
9 |
ASCII Integer |
X |
X-coordinate in FIPS FOV. |
|
|
|
|
|
|
8 |
ASCII Real |
Y |
Y-coordinate in FIPS FOV. |
|
|
|
|
|
|
16 |
ASCII Real |
V_POLAR |
Polar angle of the corresponding XY pixel. Values range 15-75. Zero is aligned with the FIPS boresight
vector |
|
54 |
ASCII Real |
V_AZIMUTH |
Azimuthal angle of the corresponding XY pixel. Values range 0-359.
Zero is aligned with the X axis in FIPS Cartesian coordinates. |
|
16 |
ASCII Real |
PIXEL_SOLID_ANG |
The solid angle viewing area of the corresponding XY pixel. |
|
16 |
ASCII Real |
PIXEL_EFF |
Relative efficiency of the corresponding XY pixel. Value is normalized by the average of
efficiencies across all visible pixels. The average of these values across
all pixels on the MCP is 1. |
|
16 |
ASCII Integer |
QUAL |
Pixel quality flag. 0 - Good pixel; 1 - SC body obstructed pixel. |
The following SPICE kernel files will be used to compute the UTC time and any geometric quantities found in the PDS labels. Kernel files will be generated throughout the mission with a file naming convention specified by the MESSENGER project.
*.bsp:
MESSENGER spacecraft ephemeris file. Also known as the Planetary Spacecraft Ephemeris Kernel (SPK) file.
*.bc:
MESSENGER spacecraft orientation file. Also known as the Attitude C-Kernel (CK) file.
*.tf:
MESSENGER reference frame file. Also known as the Frames Kernel. Contains the MESSENGER spacecraft, science instrument, and communications antennae frame definitions.
*.ti:
MESSENGER instrument kernel (I-kernel). Contains references to mounting alignment, operation modes, and timing as well as internal and field of view geometry for the EPPS.
*.tsc:
MESSENGER spacecraft clock coefficients file. Also known as the Spacecraft Clock Kernel (SCLK) file.
*.tpc:
Planetary constants file. Also known as the Planetary Constants Kernel (PcK) file.
*.tls:
NAIF leapseconds kernel file. Used
in conjunction with the SCLK kernel to convert between Universal Time
Coordinated (UTC) and MESSENGER Mission Elapsed Time (MET). Also called the
Leap Seconds Kernel (LSK) file.
CODMAC/NASA Definition of processing levels for
science data sets
|
CODMAC Level |
Proc. Type |
Data Processing
Level Description |
|
1 |
Raw Data |
Telemetry data stream as received at the ground station, with
science and engineering data embedded. Corresponds to NASA packet data. |
|
2 |
Edited Data |
Instrument science data (e.g. raw voltages, counts) at full
resolution, time ordered, with duplicates and transmission errors removed.
Referred to in the MESSENGER program as
Experiment Data Records (EDRs). Corresponds to NASA Level 0 data. |
|
3 |
Calibrated Data |
Edited data that are still in units produced by instrument, but
have transformed (e.g. calibrated, rearranged) in a reversible manner and
packaged with needed ancillary and auxiliary data (e.g. radiances with
calibration equations applied). Referred to in the MESSENGER Program as
Calibrated Data Records (CDRs). In some cases these also qualify as derived
data products (DDRs). Corresponds to NASA Level 1A. |
|
4 |
Resampled data |
Irreversibly transformed (e.g. resampled, remapped, calibrated)
values of the instrument measurements (e.g. radiances, magnetic field
strength). Referred to in the MESSENGER program as either derived data products
(DDPs) or derived analysis products (DAPs). Corresponds to NASA Level 1B. |
|
5 |
Derived Data |
Derived results such as maps, reports, graphics, etc. Corresponds to NASA Levels 2 through 5 |
|
6 |
Ancillary Data |
Non-Science data needed to generate calibrated or resampled data
sets. Consists of instrument gains, offsets; pointing information for scan
platforms, etc. |
|
7 |
Corrective Data |
Other science data needed to interpret space-borne data sets.
May include ground based data observations such as soil type or ocean buoy
measurements of wind drift. |
|
8 |
User Description |
Description of why the data were required, any peculiarities
associated with the data sets, and enough documentation to allow secondary
user to extract information from the data. |
The above
is based on the national research council committee on data management and
computation (CODMAC) data levels.
ACT Applied
Coherent Technology Corporation
ADU Analog-to-Digital
Units
AMU Atomic Mass Unit
APL The
Johns Hopkins university Applied Physics Laboratory
ASCII American
Standard Code for Information Interchange
CDR Calibrated Data Record
CK Attitude C-Kernel (SPICE)
CODMAC Committee on Data Management and Computation
DAP Derived Analysis Products
DDP Derived Data Products
DSHV Deflection System High Voltage
EDR Experiment Data Records
EPPS Energetic Particle and Plasma Spectrometer
EPS Energetic Particle Spectrometer
ESA Electrostatic Analyzer
FIFO First
In, First out. An electronic component that stores and retrieves information
following a first-in-first-out discipline.
FIPS Fast Imaging Plasma Spectrometer
FOV Field-of-View
FSW Flight Software
FTP File Transfer protocol
GEANT4 GEometry
ANd Tracking software toolkit
GF Geometric Factor
I2C Inter-Integrated Circuit
JPL Jet Propulsion Laboratory
IEM Integrated Electronic Module
LSB Least Significant Bit
LSK Leapseconds Kernel (SPICE)
MCP Micro-channel Plate
MESSENGER MErcury Surface, Space ENvironment,
GEochemistry, and Ranging
MET Mission Elapsed Time
MIDL Mission Independent Data Layer
MSO Mercury-centric Solar Orbital
NAIF Navigation and Ancillary Information Facility
NASA National Aeronautics and Space Administration
PCK Planetary Constant Kernel (SPICE)
PDS Planetary Data System
PHA Pulse Height Analysis
PPI Planetary Plasma Interactions PDS Node
RDR Reduced Data Record
SCLK Space Clock Kernel (SPICE)
SOC Science Operations Center
SPICE Spacecraft, Planet,
Instrument, C-matrix Events, refers to the kernel files and NAIF software used
to generate viewing geometry.
SPK Spacecraft and Planets Kernel (SPICE)
SSD Solid-State Detector
SSR Space Sciences Review
TOF Time of Flight
UTC Coordinated Universal Time