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'`  @K  @  'Ȁ'` @7  @ '̀+bX< `   < `  @>'bX< `  @bX< `  '`@  '< `  @< `  @'< `  bX< `   @@Ԕ@!@ΔbX< `   < `   < `  @$@㿐'& '@< `  @B㿀'''$ '@3'!$"h< `    `@y`@r   < `  @i$ !$"l!"h`' !뀤$"p!"p'!"l %`< `   $< `  @< `  '!뀤`{$"t '+bt$- $< `   @ @ 'bt$ $< `  @  @ '耤?-t  $@< `   %``$ $@< `  @%``$@֔ t $   $< `  @Ȕ$ !"t !$"l#bt? $bt#bp $bp䀤Z㿈'& '!$"x@< `  !$"|@ !뀤$"+b$a4 $< `  @  b!$"x#b $b!"x㿀'''" '@< `  '!$"' !뀤{$" '+b$-8 $< `   @>  6  'b$ $< `  @&   $  '耤;-$  @$ , < / $< `   $@ $< `  @$@@ $   $< `  @$ #b $b䀤㿀'''" '@< `  '!$"' !뀤{$" '+b$-@ $< `   @  6  'b$ $< `  @   $  '耤;-$  @ , < / $< `   $@ $< `  @a$@@Z $   $< `  @M$ #b $b䀤㾠' $'!͠ '< ?@ڐ,!$""''┪)ͨ  $''< ?@@,$'㿠 㿠*** PIMMS version 3.9i *** 2008 Nov 4rd release Reading mission directory, please waitSHOWERROR selecting spectral modelERROR selecting output missionERROR selecting output missionEnter input rate > <--- Use 'MODEL' command to change* By default, input rate is taken to be <--- Use 'FROM' command to change the default* Simulation product will be <--- Use 'INSTRUMENT' command to switch to another instrumentEnter log file name (or 'close') closeERROR:: Failed to write the current model pimms.ahl* PIMMS commands are: MODEL, FROM, INSTRUMENT, SHOW, DIRECTORY, LOG, OUTPUT, HELP and QUIT ?A bX'@ ?SEQUENTIALFORMATTEDREADONLYOLDlstpms_mssn.lstFATAL ERROR:: failed to open mission list filePIMMS was looking for 'pms_mssn.lst' inpms_intlz.f?helpPIMMS knows about the following Blackbody (BB) Powerlaw (PL) (Thermal) Bremsstrahlung (TB) RaymondSmith (RS) For the above, enter name, temperature/slope and Nh e.g., model bb 2.4 2e21also Gaussian (GA) model is availableSEQUENTIALFORMATTEDREADONLYOLDidxmodel.idxSEVERE ERROR:: failed to open model.idxPIMMS also knows about following precalculated models:#FMT(a) For these, type MODEL []PIMMS can also use any Ascii files containing: energy (kev), flux (photons/cm/cm/s) pairs as model For this, type [] For a full usage of the model command, (including multi-component models),please consult the User's Guidez Enter redshift > WARNING:: Extra numerical parameter(s) - ignoringERROR parsing parameters:: FCI is confusedbbbl Enter blackbody temperature (keV) > Enter Nh > Enter Nh > tbbr Enter bremsstrahlung temperature (keV) > Enter Nh > Enter Nh > pl Enter photon index > Enter Nh > Enter Nh > ga Enter line center energy > Enter physical width (keV) > Enter physical width (keV) > rslogtERROR parsing parameters:: FCI is confusedkevERROR parsing parameters:: FCI is confused Enter plasma temperature (keV) > Enter log10(plasma temperature) > SEQUENTIALFORMATTEDREADONLYOLDidxrs.idxConfusion in unit_code#FMTu.WARNING - this version of PIMMS has a grid of 3Q Raymond-Smith plasma models( 'WARNING - this version of PIMMS has a grid of ', i3, ' Raymond-Smith plasma models' )#FMT1 from log T of -; kT = -+( ' from log T of ', f5.2, '; kT = ', f6.3 )#FMT1 to log T of -; kT = -+( ' to log T of ', f5.2, '; kT = ', f6.3 ) choosing the nearest one, hope that's okayChoosing the nearest temperature...#FMTe New temperature is -" keV (log T is -Z)( ' New temperature is ', f6.3, ' keV (log T is ', f5.2, ')' )SEQUENTIALFORMATTEDREADONLYOLDmdlERROR: Model file buffer full!!! (Increase m_pix in pimms.inc) Enter Nh > ERROR:: Failed to open a Raymond Smith fileSEQUENTIALFORMATTEDREADONLYOLDmdl SEQUENTIALFORMATTEDREADONLYOLDmdlERROR: Model file buffer full!!! (Increase m_pix in pimms.inc)ERROR: Unknown modelValue of Nh is rather small ---Assuming that log10(Nh) was given Enter equivalent width (eV) relative to comp. 1 > Enter flux relative to comp. 1 > ...at what energy ? ...at what energy ? Warning:: Ignoring extra numerical parameter(s)Warning:: Ignoring extra numerical parameter(s)ERROR:: Cannot normalize components at this energyERROR:: Cannot normalize components at this energyWarning:: Ignoring extra numerical parameter(s)?K1@?A:o(a) 421( 'WARNING - this version of PIMMS has a grid of ', i3, ' Raymond-Smith plasma models' )422( ' from log T of ', f5.2, '; kT = ', f6.3 )423( ' to log T of ', f5.2, '; kT = ', f6.3 )440( ' New temperature is ', f6.3, ' keV (log T is ', f5.2, ')' )pms_slmdl.f Enter units (ergs or photons) > Enter integration range in keV (e.g. 2-10) > Enter units (ergs or photons) >Enter energy in keV >No mission name (or 'flux') givenType 'directory' for a list of valid mission namesAmbiguousd mission nameType 'directory' for a list of valid mission namesUnknown mission nameType 'directory' for a list of valid mission namesNo detector name givenType 'directory' for a list of valid mission namesAmbiguousd detector nameType 'directory' for a list of valid mission namesUnknown detector nameType 'directory' for a list of valid mission namesNo filter name givenType 'directory' for a list of valid mission namesAmbiguousd filter nameType 'directory' for a list of valid mission namesUnknown filter nameType 'directory' for a list of valid mission namesAmbiguous unit of flux; use ergs or photonsUnknown unit of flux; use ergs or photonsImage simulation needs a mission, not 'flux'PIMMS does not know how to calculate this data product for this instrumentERROR in PMS_SELECT:: parameter read error from XPIERROR in PMS_SELCT:: garbled energy rangeERROR in PMS_SELCT:: unexpected extra parameter is givenSEVERE ERROR in PMS_SELCT:: Mission Index is confusedAF`k?y?pms_selct.fPIMMS predicts 0.0 flux/count rate for original instrumentConversion is therefore impossible#FMT2" (Internal model normalization = ! ()(' (Internal model normalization = ',1pe10.3,')')?@ Warning:: integration from energies < calibration dataWarning:: integration to energies > calibration data B`8ѷ03,*J?AF`k$%?Warning:: integration from energies < model tableWarning:: integration to energies > model tableERROR:: Inconsistent Integration BoudariesWarning:: integration from energies < calibration dataERROR:: non-overlapping energy ranges of model and calibrationWarning:: integration to energies > calibration data(' (Internal model normalization = ',1pe10.3,')') @ pms_docrt.f@ 8ѷ8ѷEnter output file name >SEQUENTIALFORMATTEDOVERWRITENEWmdl Error opening output file Enter lowest energy of interest (keV) >Enter lowest energy of interest (keV) >ERROR in energy rangeEnter energy step (keV) >ERROR in energy step#FMT"-   !   ( f9.4, ' ', 1p, 9( e10.3, ' ' ) )@A ;o100( f9.4, ' ', 1p, 9( e10.3, ' ' ) )pms_outpt.f@A ;oAREAFATAL ERROR in PMS_RAREA:: file name cannot be foundSEQUENTIALFORMATTEDREADONLYOLDareaFATAL ERROR in PMS_RAREA:: file cannot be openedFATAL ERROR in PMS_RAREA:: file in unrecognized formatFATAL ERROR in PMS_RAREA:: too many pointspms_rarea.fSPECIALSEQUENTIALFORMATTEDREADONLYOLDSPECIAL [Count rate per single SIS, not per pair, over an entire chip assuming a point source at the 1-CCD mode position; within the maximum circular extraction region that fits on the default chip, usable rates are (3.2 arcmin radius, SIS-0) and (2.5 arcmin, SIS-1)]#FMT- (f9.1)#FMT ! (1p,e9.2)#FMT- (f9.1)#FMT ! (1p,e9.2)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range [Count rate per single GIS, not per pair, but over the entire detector. For point source at the 1-CCD mode position and a 24 pixel (6 arcmin) extraction radius, usable rates are (GIS2) and (GIS3)]#FMT- (f9.1)#FMT ! (1p,e9.2)#FMT- (f9.1)#FMT ! (1p,e9.2)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range (Count rate is per PCU)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range (Source-only count rate in 1 cluster)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range (Source-only count rate for a single SSC, with the source on-axis) (Count rate in Levin et al (1984, ApJS 54, 581) band A+B+C)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range (Source count rate for 2 MECS)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Pileup estimate for ACIS:% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Pileup estimate for ACIS: (=Sum of source count rates in +1st and -1st orders) for on-axis observation before dead time correction and assuming a 15 arcsec extraction radius (the total source count rate is approx. 47% higher)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy rangeWARNING: MOS1 Timing mode data now suffers from an out-of-scale columnwhich results in 20-30% loss of counts for sources at the nominal position. for on-axis observation before dead time correction, PATTERN=0 only rate assuming a 15 arcsec extraction radius (the total PATTERN=0 count rate is approx. 47% higher)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy rangeWARNING: The pile-up estimate is approximate% This estimate is appropriate for a point source centerd on the array% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Event grade split estimates are:% This estimate is appropriate for a point source centerd on the array% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Event grade split estimates are: (count rate per FI XIS) (for a point source at the "XIS nominal" pointing position) (Count rate at the "HXD nominal" pointing position is ~10% lower) (correction for the 5.6% dead area created by charge injection included) (for a point source at the "XIS nominal" pointing position) (Count rate at the "HXD nominal" pointing position is ~10% lower) (correction for the 7.4% dead area created by charge injection included) (for a point source at the "XIS nominal" pointing position) (Count rate at the "HXD nominal" pointing position is ~10% higher)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range (Channel 3-78 count rate per fully illuminated detector)% Further instrument-specific information can be obtained by re-running PIMMS without specifying a limited (non-default) energy range (Grade 0-12 on-axis count rate for an infinite extraction region) or cps in Grade 0#FMT ! (1p,e10.3) (Greade 0-2 on-axis count rate for an infinite extraction region) or cps in Grade 0#FMT ! (1p,e10.3) (Grade 0-5 on-axis count rate for an infinite extraction region) or cps in Grade 0-2#FMT ! (1p,e10.3) or cps in Grade 0#FMT ! (1p,e10.3)?H$pms_specl.f(f9.1) (1p,e9.2) (f9.1) (1p,e9.2) (f9.1) (1p,e9.2) (f9.1) (1p,e9.2) (1p,e10.3) (1p,e10.3) (1p,e10.3) (1p,e10.3) SPECIALSEQUENTIALFORMATTEDREADONLYOLDSPECIAL%!% Integration over the entire chip (not just in the source region) assumed%!% Integration over full GIS FOV (not just in the source region) assumed%!% Count rate is assumed to be per PCU%!% Net count rate per cluster assumed%!% Count rate assumed to be for 2 MECS%!% No pile-up correction will be applied%!% Count rate assumed to be sum of +/-1st orders%!% Pile-up corrected rate in 15 arcsec region assumed%!% Pile-up corrected PATTERN=0 only rate in 15 arcsec region assumed%!% Count rate per 1 FI unit assumed%!% Observation at "XIS Nominal" pointing position assumed%!% Source count rate (channels 3-78) per fully illuminated detector assumed%!% Total (not just source region) Grade 0-12 count rate assumed%!% Total (not just source region) Grade 0-2 count rate assumed%!% Total (not just source region) Grade 0-5 count rate assumedpms_spec2.f#FMTY Unabsorbed flux (- 8-- C keV) in V( ' Unabsorbed flux (', f9.3, '-', f9.3, ' keV) in ', a )#FMTY Unabsorbed flux (- :-- E A) in V( ' Unabsorbed flux (', f9.5, '-', f9.5, ' A) in ', a )#FMT. Flux (-  --  keV) in +( ' Flux (', f9.3, '-', f9.3, ' keV) in ', a )#FMT, Flux (-  --  A) in )( ' Flux (', f9.5, '-', f9.5, ' A) in ', a )#FMTa Unabsorbed flux density @- EkeV in V/keV( ' Unabsorbed flux density @', f9.3, 'keV in ', a, '/keV' )#FMTa Unabsorbed flux density @- IA in X/A( ' Unabsorbed flux density @', f9.5, 'A in ', a, '/A' )#FMT1 Flux density @- keV in &/keV( ' Flux density @', f9.3, 'keV in ', a, '/keV' )#FMT- Flux Density @- A in $/A( ' Flux Density @', f9.5, 'A in ', a, '/A' )Model normalizationERROR in PMS_WTSLC:: instrument name cannot be found#FMT  Count rate in ( ' Count rate in ', a )#FMTX Count rate in  (- >-- I keV)( ' Count rate in ', a, ' (', 0p, f9.3, '-', f9.3, ' keV)' )#FMTV Count rate in  (- >-- I A)( ' Count rate in ', a, ' (', 0p, f9.5, '-', f9.5, ' A)' )AF`k#FMT%m and an unabsorbed flux (- !-- HkeV) of ! ^ j( ' and an unabsorbed flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )#FMT%m and an unabsorbed flux (- !-- JA) of ! ^ j( ' and an unabsorbed flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )#FMT(r%* PIMMS predicts an unabsorbed flux (- +-- MkeV) of ! c o( '* PIMMS predicts an unabsorbed flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )#FMT(r%* PIMMS predicts an unabsorbed flux (- +-- OA) of ! c o( '* PIMMS predicts an unabsorbed flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )#FMT"g and a flux (- --  keV) of ! X d( ' and a flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )#FMT"g and a flux (- --  A) of ! X d( ' and a flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )#FMT%e* PIMMS predicts a flux (- -- @keV) of ! V b( '* PIMMS predicts a flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )#FMT%f* PIMMS predicts a flux (- -- CA) of ! W c( '* PIMMS predicts a flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )#FMT#p# and an unabsorbed flux density @- )keV of ! Y e/keV( ' and an unabsorbed flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )#FMT#p# and an unabsorbed flux density @- )A of ! [ g/A( ' and an unabsorbed flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )#FMT&t-* PIMMS predicts an unabsorbed flux density @- HkeV of ! ] i/keV( '* PIMMS predicts an unabsorbed flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )#FMT&q-* PIMMS predicts an unabsorbed flux density @- IA of ! \ h/A( '* PIMMS predicts an unabsorbed flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )#FMT d and a flux density @- keV of ! M Y/keV( ' and a flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )#FMT d and a flux density @- A of ! O [/A( ' and a flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )#FMT#n!* PIMMS predicts a flux density @- 'keV of ! W c/keV( '* PIMMS predicts a flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )#FMT#n!* PIMMS predicts a flux density @- 'A of ! Y e/A( '* PIMMS predicts a flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' ) ERROR in PMS_WTINT:: instrument name cannot be found#FMT& and !  cps in #( ' and ', 1p, e10.3, ' cps in ', a )#FMTa* PIMMS predicts !  cps with ^( '* PIMMS predicts ', 1p, e10.3, ' cps with ', a )#FMT%e and !  cps in # (- L-- WkeV)( ' and ', 1p, e10.3, ' cps in ', a, ' (', 0p, f9.3, '-', f9.3, 'keV)' )#FMT)q* PIMMS predicts !  cps with K (- X-- ckeV)( '* PIMMS predicts ', 1p, e10.3, ' cps with ', a, ' (', 0p, f9.3, '-', f9.3, 'keV)' )#FMT%g and !  cps in # (- P-- [A)( ' and ', 1p, e10.3, ' cps in ', a, ' (', 0p, f9.5, '-', f9.5, 'A)' )#FMT)q* PIMMS predicts !  cps with M (- Z-- eA)( '* PIMMS predicts ', 1p, e10.3, ' cps with ', a, ' (', 0p, f9.5, '-', f9.5, 'A)' )#FMTi"* Current model is BLACKBODY, kT= -I keV; NH = ! b( '* Current model is BLACKBODY, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTk* For Blackbody model with kT=-$ keV; NH = ! d( '* For Blackbody model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTi" plus BLACKBODY, kT= -I keV; NH = ! b( ' plus BLACKBODY, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTk + Blackbody model with kT=-$ keV; NH = ! d( ' + Blackbody model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTn'* Current model is BREMSSTRAHLUNG, kT= -N keV; NH = ! g( '* Current model is BREMSSTRAHLUNG, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTr+* For thermal Bremsstrahlung model with kT=-R keV; NH = ! k( '* For thermal Bremsstrahlung model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTn' plus BREMSSTRAHLUNG, kT= -N keV; NH = ! g( ' plus BREMSSTRAHLUNG, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )#FMTr+ + thermal Bremsstrahlung model with kT=-R keV; NH = ! k( ' + thermal Bremsstrahlung model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )#FMT l%* Current model is POWER LAW, Photon Index = -P; NH = ! e( '* Current model is POWER LAW, Photon ', 'Index = ', f7.4, '; NH = ', 1p, e10.3 )#FMTp)* For power law model with photon index =-T; NH = ! i( '* For power law model with photon index =', f7.4, '; NH = ', 1p, e10.3 )#FMT l% plus POWER LAW, Photon Index = -P; NH = ! e( ' plus POWER LAW, Photon ', 'Index = ', f7.4, '; NH = ', 1p, e10.3 )#FMTp) + power law model with photon index =-T; NH = ! i( ' + power law model with photon index =', f7.4, '; NH = ', 1p, e10.3 )#FMT%k&* Current model is CUTOFF PL, Index = -:, Ecut -K keV; NH = ! d( '* Current model is CUTOFF PL, Index = ', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )#FMT$m"* For cutoff pl model with index =-(, Ecut -M keV; NH = ! f( '* For cutoff pl model with index =', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )#FMT%k& plus CUTOFF PL, Index = -:, Ecut -K keV; NH = ! d( ' plus CUTOFF PL, Index = ', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )#FMT$m" + cutoff pl model with index =-(, Ecut -M keV; NH = ! f( ' + cutoff pl model with index =', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )* Current model is power-law with high-energy cut-off#FMT)d Index = -, Ecut -! keV, E(e-folding) -D keV; NH = ! ]( ' Index = ', f5.2, ', Ecut ', f7.2, ' keV, E(e-folding) ', f7.2, ' keV; NH = ', 1p, e10.3 )* For power-law model with high-energy cut-off with plus power-law with high-energy cut-off + power-law model with high-energy cut-off with#FMT'h"* Current model is RAYMOND SMITH, kT=-6 keV (logT=-K); NH = ! a( '* Current model is RAYMOND SMITH, ', 'kT=', f7.4, ' keV (logT=', f5.2, '); NH = ', 1p, e10.3 )#FMT$o"* For Raymond Smith model with kT=-( keV (logT=-R); NH = ! h( '* For Raymond Smith model with kT=', f7.4, ' keV (logT=', f5.2, '); NH = ', 1p, e10.3 )#FMT'i" plus RAYMOND SMITH, kT= -7 keV (logT=-L); NH = ! b( ' plus RAYMOND SMITH, ', 'kT= ', f8.4, ' keV (logT=', f3.1, '); NH = ', 1p, e10.3 )#FMT$o" + Raymond Smith model with kT=-( keV (logT=-R); NH = ! h( ' + Raymond Smith model with kT=', f7.4, ' keV (logT=', f5.2, '); NH = ', 1p, e10.3 )#FMT$f* Current model is GAUSSIAN, E=-0 keV; sigma=-F keV; NH = ! _( '* Current model is GAUSSIAN, E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )#FMT#i* For Gaussian model with E=-" keV; sigma=-I keV; NH = ! b( '* For Gaussian model with E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )#FMT$f plus GAUSSIAN, E=-0 keV; sigma=-F keV; NH = ! _( ' plus GAUSSIAN, E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )#FMT#i + Gaussian model with E=-" keV; sigma=-I keV; NH = ! b( ' + Gaussian model with E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )#FMT  * Model from ( '* Model from ', a )#FMT  * For model ( '* For model ', a )#FMT  plus ( ' plus ', a )#FMT  + ( ' + ', a )#FMT, * Model from ; NH = ! %( '* Model from ', a, '; NH = ', 1p, e10.3 )#FMT+ * For model ; NH = ! $( '* For model ', a, '; NH = ', 1p, e10.3 )#FMT, plus ; NH = ! %( ' plus ', a, '; NH = ', 1p, e10.3 )#FMT+ + ; NH = ! $( ' + ', a, '; NH = ', 1p, e10.3 )#FMT4 (Eq.W=-& eV)( ' (Eq.W=', f8.4, ' eV)' )#FMTu (- times component 1 at - e keV)( ' (', f8.4, ' times component 1 at ', f10.4, ' keV)' )#FMT" ...redshifted with z=-( ' ...redshifted with z=', f8.4 )#FMTR ...redshifted with z=- and a Galactic Nh=! K( ' ...redshifted with z=', f8.4, ' and a Galactic Nh=', 1p, e10.3 )?101( ' Unabsorbed flux (', f9.3, '-', f9.3, ' keV) in ', a )102( ' Unabsorbed flux (', f9.5, '-', f9.5, ' A) in ', a )106( ' Flux (', f9.3, '-', f9.3, ' keV) in ', a )107( ' Flux (', f9.5, '-', f9.5, ' A) in ', a )111( ' Unabsorbed flux density @', f9.3, 'keV in ', a, '/keV' )112( ' Unabsorbed flux density @', f9.5, 'A in ', a, '/A' )116( ' Flux density @', f9.3, 'keV in ', a, '/keV' )117( ' Flux Density @', f9.5, 'A in ', a, '/A' )121( ' Count rate in ', a )141( ' Count rate in ', a, ' (', 0p, f9.3, '-', f9.3, ' keV)' )142( ' Count rate in ', a, ' (', 0p, f9.5, '-', f9.5, ' A)' )pms_write.f101( ' and an unabsorbed flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )102( ' and an unabsorbed flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )106( '* PIMMS predicts an unabsorbed flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )107( '* PIMMS predicts an unabsorbed flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )111( ' and a flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )112( ' and a flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )116( '* PIMMS predicts a flux (', f9.3, '-', f9.3, 'keV) of ', 1p, e10.3, ' ', a )117( '* PIMMS predicts a flux (', f9.5, '-', f9.5, 'A) of ', 1p, e10.3, ' ', a )201( ' and an unabsorbed flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )202( ' and an unabsorbed flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )206( '* PIMMS predicts an unabsorbed flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )207( '* PIMMS predicts an unabsorbed flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )211( ' and a flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )212( ' and a flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )216( '* PIMMS predicts a flux density @', f9.3, 'keV of ', 1p, e10.3, ' ', a, '/keV' )217( '* PIMMS predicts a flux density @', f9.5, 'A of ', 1p, e10.3, ' ', a, '/A' )121( ' and ', 1p, e10.3, ' cps in ', a )122( '* PIMMS predicts ', 1p, e10.3, ' cps with ', a )141( ' and ', 1p, e10.3, ' cps in ', a, ' (', 0p, f9.3, '-', f9.3, 'keV)' )142( '* PIMMS predicts ', 1p, e10.3, ' cps with ', a, ' (', 0p, f9.3, '-', f9.3, 'keV)' )161( ' and ', 1p, e10.3, ' cps in ', a, ' (', 0p, f9.5, '-', f9.5, 'A)' )162( '* PIMMS predicts ', 1p, e10.3, ' cps with ', a, ' (', 0p, f9.5, '-', f9.5, 'A)' )101( '* Current model is BLACKBODY, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )102( '* For Blackbody model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )106( ' plus BLACKBODY, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )107( ' + Blackbody model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )111( '* Current model is BREMSSTRAHLUNG, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )112( '* For thermal Bremsstrahlung model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )116( ' plus BREMSSTRAHLUNG, kT= ', f8.4, ' keV; NH = ', 1p, e10.3 )117( ' + thermal Bremsstrahlung model with kT=', f8.4, ' keV; NH = ', 1p, e10.3 )121( '* Current model is POWER LAW, Photon ', 'Index = ', f7.4, '; NH = ', 1p, e10.3 )122( '* For power law model with photon index =', f7.4, '; NH = ', 1p, e10.3 )126( ' plus POWER LAW, Photon ', 'Index = ', f7.4, '; NH = ', 1p, e10.3 )127( ' + power law model with photon index =', f7.4, '; NH = ', 1p, e10.3 )131( '* Current model is CUTOFF PL, Index = ', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )132( '* For cutoff pl model with index =', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )136( ' plus CUTOFF PL, Index = ', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )137( ' + cutoff pl model with index =', f5.2, ', Ecut ', f7.2, ' keV; NH = ', 1p, e10.3 )141( ' Index = ', f5.2, ', Ecut ', f7.2, ' keV, E(e-folding) ', f7.2, ' keV; NH = ', 1p, e10.3 )151( '* Current model is RAYMOND SMITH, ', 'kT=', f7.4, ' keV (logT=', f5.2, '); NH = ', 1p, e10.3 )152( '* For Raymond Smith model with kT=', f7.4, ' keV (logT=', f5.2, '); NH = ', 1p, e10.3 )156( ' plus RAYMOND SMITH, ', 'kT= ', f8.4, ' keV (logT=', f3.1, '); NH = ', 1p, e10.3 )157( ' + Raymond Smith model with kT=', f7.4, ' keV (logT=', f5.2, '); NH = ', 1p, e10.3 )161( '* Current model is GAUSSIAN, E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )162( '* For Gaussian model with E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )166( ' plus GAUSSIAN, E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )167( ' + Gaussian model with E=', f8.4, ' keV; sigma=', f7.4, ' keV; NH = ', 1p, e10.3 )171( '* Model from ', a )172( '* For model ', a )176( ' plus ', a )177( ' + ', a )181( '* Model from ', a, '; NH = ', 1p, e10.3 )182( '* For model ', a, '; NH = ', 1p, e10.3 )186( ' plus ', a, '; NH = ', 1p, e10.3 )187( ' + ', a, '; NH = ', 1p, e10.3 )191( ' (Eq.W=', f8.4, ' eV)' )192( ' (', f8.4, ' times component 1 at ', f10.4, ' keV)' )201( ' ...redshifted with z=', f8.4 )202( ' ...redshifted with z=', f8.4, ' and a Galactic Nh=', 1p, e10.3 )AREASEQUENTIALFORMATTEDREADONLYOLDareaSPECIALSEQUENTIALFORMATTEDREADONLYOLDSPECIAL __. Mission #FMT'Mission   with3 detectors('Mission ',a,' with',i2,' detectors') Detector #FMT( Detector  with 3 filters(' Detector ',a,' with ',i2,' filters') Filter ERROR in PDX_SHLST:: PIMMS is confusedMission #FMT# has 3 detectors.(' has ', I2, ' detectors.') Detector #FMT# has 3 filters.(' has ', I2, ' filters.') Filter ERROR in PDX_SHLST:: PIMMS is confused Detector #FMT# has 3 filters.(' has ', I2, ' filters.') Filter Images can be simulatedImages can be simulatedImages can be simulatedInstrument specific information is availableInstrument specific information is availableInstrument specific information is availablepms_index.f('Mission ',a,' with',i2,' detectors') (' Detector ',a,' with ',i2,' filters')(' has ', I2, ' detectors.') (' has ', I2, ' filters.') (' has ', I2, ' filters.') Mission name unknown, giving full directory listingDetector name unknown #FMT(a)(a) pms_colmn.f * The source is apparently too bright for SIS If this is unexpected, check the unit of input rate* It appears to take more than 10 million s for a 5-sigma detection#FMTv* An exposure of - s is required for a 5-sigma detection using optimal( '* An exposure of ', f10.2, 's is required for a', ' 5-sigma detection using optimal' )#FMT'u extraction radius of - arcmin (! O src and ! b bgd cps)( ' extraction radius of ', f4.2, ' arcmin (', 1p, e9.2, ' src and ', e9.2, ' bgd cps)' ) * Extrapolated to 1998 Dec for S1C3 in 1-CCD mode at 2 SIS temperatures: #FMT,n Telemetry is -% full, -'% full, -C % full, and -Y% full  j( ' Telemetry is ', f4.1, '% full, ', f4.1, '% full, ', f4.1, '% full, and ', f4.1, '% full ', a9 )#FMT'h Telemetry is saturated, -!% full, -= % full, and -S% full  d( ' Telemetry is saturated, ', f4.1, '% full, ', f4.1, '% full, and ', f4.1, '% full ', a9 )#FMT"h Telemetry is saturated, -!% full, saturated, and -S% full  d( ' Telemetry is saturated, ', f4.1, '% full, saturated, and ', f4.1, '% full ', a9 )#FMT m& Telemetry is saturated, saturated, saturated, and -X% full  i( ' Telemetry is saturated, saturated,', ' saturated, and ', f4.1, '% full ', a9 ) Telemetry is saturated, saturated, saturated, and saturated in Faint (M), Faint (H), Bright (M), and Bright (H) modes (S0C1 has lower flickering pixel rate; decide modes based on S1C3)F@4c@<KABBCBf105( '* An exposure of ', f10.2, 's is required for a', ' 5-sigma detection using optimal' )106( ' extraction radius of ', f4.2, ' arcmin (', 1p, e9.2, ' src and ', e9.2, ' bgd cps)' )110( ' Telemetry is ', f4.1, '% full, ', f4.1, '% full, ', f4.1, '% full, and ', f4.1, '% full ', a9 )111( ' Telemetry is saturated, ', f4.1, '% full, ', f4.1, '% full, and ', f4.1, '% full ', a9 )112( ' Telemetry is saturated, ', f4.1, '% full, saturated, and ', f4.1, '% full ', a9 )113( ' Telemetry is saturated, saturated,', ' saturated, and ', f4.1, '% full ', a9 )4c@sis_limit.fSEQUENTIALFORMATTEDREADONLYOLDdatasca_sis_psf.datSEVERE ERROR:: Datafile not found@sis_obstm.f Telemetry will be saturated, saturated, and saturated in H, M and L bit rate#FMT -% full(f3.1,'% full')#FMT -% full(f3.1,'% full')#FMT -% full(f3.1,'% full')#FMT -% full(f3.1,'% full')#FMT -% full(f3.1,'% full')#FMT 3% full(i3,'% full')#FMT -% full(f3.1,'% full')#FMT 3% full(i3,'% full')#FMT 3% full(i3,'% full')#FMT -% full(f3.1,'% full')#FMT 3% full(i3,'% full')#FMT 3% full(i3,'% full')#FMT 3% full(i3,'% full')#FMT 3% full(i3,'% full') using PH mode (MPC mode is not recommended) allowing for ~1 cps for X-ray and particle background and the on-board calibration source.CBA@>?AL(f3.1,'% full') (f3.1,'% full') (f3.1,'% full') (f3.1,'% full') (f3.1,'% full') (i3,'% full') (f3.1,'% full') (i3,'% full') (i3,'% full') (f3.1,'% full') (i3,'% full') (i3,'% full') (i3,'% full') (i3,'% full') gis_limit.f% In the 15-40 keV band, PIMMS predicts n.nnnE+mm source cps, n.nnnn CXB cps, and n.nnnn NXB cps#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3)#FMT-(f6.4)#FMT-(f6.4) The source is undetectable at 3-sigma The source is detectable at 3-sigma in n.nnnE+nn s#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3) The source is undetectable at 5-sigma The source is detectable at 5-sigma in n.nnnE+nn s#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3) The source is undetectable at 3-sigma (considering the x.x% systematic uncertainty in the NXB estimation)#FMT-(f3.1)E@<# ? B`AAB% In the nnn-nnn keV band, PIMMS predicts n.nnnE+mm source cps and nn.nnn NXB cps#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3)#FMT-(f6.3) The source is undetectable at 3-sigma The source is detectable at 3-sigma in n.nnnE+nn s#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3) The source is undetectable at 5-sigma The source is detectable at 5-sigma in n.nnnE+nn s#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3) The source is undetectable at 3-sigma (considering the x.xx% systematic uncertainty in the NXB estimation)#FMT-(f4.2)@(1p,e9.3) (f9.3) (1p,e9.3) (f6.4) (f6.4) (1p,e9.3) (f9.3) (1p,e9.3) (1p,e9.3) (f9.3) (1p,e9.3) (f3.1) hxd_limit.f(1p,e9.3) (f9.3) (1p,e9.3) (f6.3) (1p,e9.3) (f9.3) (1p,e9.3) (1p,e9.3) (f9.3) (1p,e9.3) (f4.2) SEVERE ERROR:: PIMMS is confused in HXT_LIMITSEVERE ERROR:: PIMMS is confused in HXT_LIMIT (Source-only count rate in 1 cluster; BGD rate is 34.4 per cluster)#FMT-(f5.1)Predicted count rate very high: mistake maybe?5-sigma detection will be achieved in s#FMT ! (1p,e9.2)#FMT- (f9.1)#FMT ! (1p,e9.2)Count rate too low: 5-sigma detection impossible Results in the 4 canonical XTE HEXTE bands are: (per HEXTE cluster) Channels Nominal Source BGD 5-sigma E (keV) (cps) (cps) detection (s) 0- 29 30- 30 0.0 0.0 ********#FMT ! (1p,e9.2)#FMT-(f5.1)#FMT ! (1p,e9.2)#FMT-(f6.2) ********#FMT ! (1p,e9.2)#FMT- (f9.1)#FMT ! (1p,e9.2) ******** (The default 16-s rocking cycle is assumed for detection time)AXc_@H$?C(f5.1) (1p,e9.2) (f9.1) (1p,e9.2) (1p,e9.2) (f5.1) (1p,e9.2) (f6.2) (1p,e9.2) (f9.1) (1p,e9.2) hxt_limit.fSEVERE ERROR:: PIMMS is confused in PCA_LIMITPredicted count rate very high: mistake maybe? %%% With 3 PCUs operational: (Use these numbers in RPS) %%% ...and with 2 PCUs operational: Xc_@@<# @PIMMS predicts n.nnnE+mm cps from the source plus n.nnnE+mm background cps#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)5-sigma detection will be achieved in s#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)(or in s with 1% systematic uncertainties in bgd)#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)(but undetectable with 1% systematic uncertainties in bgd)Count rate too low: 5-sigma detection unlikely Results in the 6 canonical XTE PCA bands are: Channels Nominal Source BGD 5-sigma (+1%) E (keV) (cps) (cps) detection (s)( )#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)#FMT-(f6.2) *****************#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2)********* *****************E@ B`A@@@<# @<# (1p,e9.2) (f9.3) (1p,e9.2) (1p,e9.2) (f9.3) (1p,e9.2) (1p,e9.2) (f9.3) (1p,e9.2) (1p,e9.2) (f9.3) (1p,e9.2) (1p,e9.2) (f9.3) (1p,e9.2) (f6.2) (1p,e9.2) (f9.3) (1p,e9.2) (1p,e9.2) (f9.3) (1p,e9.2) pca_limit.fSEVERE ERROR:: PIMMS is confused in HA4_LEVIN Results in the 4 Levine et al bands are: Levine Nominal Source Band E (keV) (cps)#FMT ! (1p,e9.2)#FMT- (f9.1)#FMT ! (1p,e9.2)H$?(1p,e9.2) (f9.1) (1p,e9.2) ha4_levin.f * Results in 2 SAX LECS bands are:* Band Source BGD 5-sigma* keV cps cps detection (s) 0.1-10#FMT-- - (a7,f7.3,3x,f7.3,3x,f10.2) 0.1-1 * Assumed 8 arcmin radius (95 % source region at 0.284 keV)* 0.1-10 keV bgd rate of 0.025 cps for 1 LECS#FMT_* An exposure of - %s is required for a 5-sigma detection( '* An exposure of ', f10.2, 's is required for a 5-sigma detection' ) * Assumed 4 arcmin radius (90 % source region at 5 keV)* 2-10 keV bgd rate of 0.0058 cps for 2 MECS * Results in 4 SAX PDS bands are:* Band Source BGD 5-sigma* keV cps cps detection (s) 13-200 13-30 30-80 80-200 * !!!NOTE!!! that using the PDS in the standard rocking mode half of the observing time is allocated to monitor the bgd * Results in 3 SAX HPGSPC bands are:* Band Source BGD 5-sigma* keV cps cps detection (s) 4-120 4-34 34-120 * !!!NOTE!!! that using the HPGSPC in the standard rocking mode half of the observing time is allocated to monitor the bgdno Special for now@:=;o?L<; ?}p@;9w:ѷ; ?s33B33@A33A@A@A333BBHB201( '* An exposure of ', f10.2, 's is required for a 5-sigma detection' )401(a7,f7.3,3x,f7.3,3x,f10.2)sax_limit.f The input frame time is out of sensible range For a frame time of s, #FMT-(f5.3)the count rate after pile-up is #FMT ! (1p,e10.3)#FMT- (f10.5)#FMT ! (1p,e10.3) (or a pile-up fraction of %)#FMT-(f7.3) Pile-up is not significant (#FMT-(f6.3) %) at normal frame-time (3.2s)#FMT-(f3.1) Pile-up is tolerable ( %)#FMT-(f4.1) at a frame-time of s#FMT-(f6.3) Pile-up is too high ( %) at the #FMT-(f4.1)fastest single-chip frame time (0.2 s)#FMT-(f3.1) Consider using the Continuous Clocking mode@L>LB:oA =? The count rate after pile-up is #FMT ! (1p,e10.3)#FMT- (f10.5)#FMT ! (1p,e10.3) (3.2 s frame time assumed)#FMT-(f3.1) (or a pile-up fraction of %)#FMT-(f7.3)?=x(f5.3) (1p,e10.3) (f10.5) (1p,e10.3) (f7.3) (f6.3) (f3.1) (f4.1) (f6.3) (f4.1) (f3.1) acis_pileup.f@L>L(1p,e10.3) (f10.5) (1p,e10.3) (f3.1) (f7.3) @L % Pile-up and dead-time corrected count rates in 4 energy bands using various window options are: Window Pileup Dead Corrected Good Count Rates Option frac. Time 0.1-0.4 0.4-1.0 1.0-2.5 2.5-10.0 Total <0.001%#FMT -%(F6.3,'%')#FMT -%(F4.1,'%')-------0.0% ?(B<# :o? % Pile-up and dead-time corrected count rates in 4 energy bands using various window options are: Window Pileup Dead Corrected Good Count Rates Option frac. Time 0.1-0.4 0.4-1.0 1.0-2.5 2.5-10.0 Total >10%<0.001%#FMT -%(F6.3,'%')>10%#FMT -%(F4.1,'%')?-------#FMT -%(F4.1,'%')-------#FMT -%(F4.1,'%') % Any pile-up predictions over 10% are highly uncertain @]A =* For >=100% pile-up calculated, check the numbers? Pile-up is predicted to be <0.001%#FMT, Pile-up is predicted to be -"%(' Pile-up is predicted to be ', f6.3, '%') in the FULL window mode. % In window mode The rate is FULL mode rate * 0.00183 = #FMT-(f7.5)#FMT ! (1p,e10.3)#FMT- (f10.5)#FMT ! (1p,e10.3)Dz* >=100% pile-up calculated, check the numbers?* Pile-up is predicted to be <0.001%#FMT,* Pile-up is predicted to be -"%('* Pile-up is predicted to be ', f6.3, '%')#FMT ! (1P,E9.2)#FMT- (F9.4)#FMT ! (1P,E9.2)Dy(F6.3,'%') (F4.1,'%') epic_pileup.f(F6.3,'%') (F4.1,'%') (F4.1,'%') (F4.1,'%') (' Pile-up is predicted to be ', f6.3, '%')(f7.5) (1p,e10.3) (f10.5) (1p,e10.3) ('* Pile-up is predicted to be ', f6.3, '%')(1P,E9.2) (F9.4) (1P,E9.2) Filter Hi-Res Hi+Med Res Med (S) Low-ResOpenND (10%) (For a total of ct/s with the 10% ND filter)#FMT ! (1p,e9.3)#FMT- (f9.4)Be=,=F@#FMT ! (1p,e9.3)#FMT- (f9.4)#FMT ! (1p,e9.3)#FMT- (f9.4)#FMT ! (1p,e9.3)#FMT- (f9.4)#FMT ! (1p,e9.3)#FMT- (f9.4)Telemetry Saturation (160 c/s)?C ?ff<-`DMA?PbMD ׮C&b}?< @)j?I@<\࿯? y(1p,e9.3) (f9.4) xrs_pileup.f(1p,e9.3) (f9.4) (1p,e9.3) (f9.4) (1p,e9.3) (f9.4) (1p,e9.3) (f9.4) Predicted rate very high: mistake maybe?ERROR:: Instrument code unrecognizedERROR:: Mismatch in number of sub-bands%%% in the band#FMT] !   source c/s +-D background c/s( ' ', 1p, e9.2, ' source c/s +', 0p, f6.1, ' background c/s' )#FMTU -  source c/s +-< background c/s( ' ', f9.3, ' source c/s +', f6.1, ' background c/s' ) 3-sigma detection will be achieved in s#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2) (or in s with 2% systematic uncertainties in bgd)#FMT ! (1p,e9.2)#FMT- (f9.3)#FMT ! (1p,e9.2) (but undetectable with 2% systematic uncertainties in bgd) Count rate too low: 3-sigma detection unlikelyXc_E@<# B`A< @@111( ' ', 1p, e9.2, ' source c/s +', 0p, f6.1, ' background c/s' )112( ' ', f9.3, ' source c/s +', f6.1, ' background c/s' )(1p,e9.2) (f9.3) (1p,e9.2) (1p,e9.2) (f9.3) (1p,e9.2) int_limit.fSEVERE ERROR:: PIMMS is confused in BAT_LIMITPredicted count rate very high: mistake maybe? With nnnn.n background cps, it can be detected at S/N=abc in n.nnnE+mm s#FMT-(f6.4)#FMT-(f3.1)#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3) Results in the 4 standard Swift/BAT survey bands are: Channel / Energy Source BGD Detection 1-3 keV n.nnnE+mm ffff.f n.nnnE+mm s#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3)#FMT-(f6.4)#FMT ! (1p,e9.3)#FMT- (f9.3)#FMT ! (1p,e9.3)DzA@>\)G@E@<# (f6.4) (f3.1) (1p,e9.3) (f9.3) (1p,e9.3) (1p,e9.3) (f9.3) (1p,e9.3) (f6.4) (1p,e9.3) (f9.3) (1p,e9.3) bat_limit.f- .09.-+eEdDeEdD09#FMT (i3)('(i',i2,')')#FMT (i3)('(i',i1,')')09-+.09#FMT(f3.3 )('(f',i2,'.',i2,')')#FMT(f3.3 )('(f',i2,'.',i1,')')#FMT(f3.3 )('(f',i1,'.',i1,')').09.0-+9#FMT(e3.3 )('(e',i2,'.',i2,')')#FMT(e3.3 )('(e',i2,'.',i1,')')#FMT(e3.3 )('(e',i1,'.',i1,')')('(i',i2,')') ('(i',i1,')') ('(f',i2,'.',i2,')')('(f',i2,'.',i1,')')('(f',i1,'.',i1,')')('(e',i2,'.',i2,')')('(e',i2,'.',i1,')')('(e',i1,'.',i1,')')rd_real.fERROR in SIMP32:: reverse boundary=?@@>ERROR in SIMP2K:: reverse boundarySIMP2K Warning:: Taking too long to converge, cutting at n=131072 the result may be somewhat inaccurate.ERROR in SPEC:: Model number incorrectB?B3b1H|? #A0p_@2\@ >?@ lspec.f<^~8ѷ`xp??TPSoG;"y_m_FCI FATAL ERROR: Too many commands, cannot initializeFCI FATAL ERROR: Prompt string too long to initializeFCI FATAL ERROR: Too many commands, cannot initialize #FMT(A)! #FMT(A256);FCI ERROR:: Illegal command separator$@FCI ERROR:: already reading from a fileSEQUENTIALFORMATTEDREADONLYOLDxco FCI ERROR:: Failed to open command file?; ; #FMT]!FCI WARNING:: Command too long... truncated to 3M letters( 'FCI WARNING:: Command too long...', 'truncated to ', i2, ' letters' ); ''; ' #FMT. FCI ERROR:: Ambiguous command: "&"( 'FCI ERROR:: Ambiguous command: "', A, '"' )#FMT,FCI ERROR:: Unknown command :"$"( 'FCI ERROR:: Unknown command :"', A, '"' )(A) (A256) 110( 'FCI WARNING:: Command too long...', 'truncated to ', i2, ' letters' )310( 'FCI ERROR:: Ambiguous command: "', A, '"' )320( 'FCI ERROR:: Unknown command :"', A, '"' )getcom.fFCI WARNING:: Too many integer parameters...ignoring oneFCI WARNING:: Too many floating-number parameters...ignoring one FCI WARNING:: Too many character string parameters...ignoring one''''FCI WARNING:: Character string too long...truncatingFCI WARNING:: Character string is too long...truncating set_param.fERROR:: non-positive number not allowedERROR in GET_PARAM_C:: Trying to access a non-existent parameter ERROR in GET_PARAM_C:: parameter is too long...truncatingERROR:: non-positive number not allowed ERROR in GET_PARAM_F:: Trying to access a non-existent parameterERROR:: non-positive number not allowed ERROR in GET_PARAM_I:: Trying to access a non-existent parameterERROR:: non-positive number not allowed ERROR in GET_PARAM_N:: Trying to access a non-existent parameterERROR in GT2_PARAM_N:: Trying to access a non-existent parameter! #FMT(a)#FMT(a)#FMT(a)! get_param.f(a) (a) (a) FCI FATAL ERROR:: Command line too longFCI FATAL ERROR:: Command buffer overload DIRECTUNFORMATTEDREADONLYOLDAHLSEVERE ERROR:: Failed to open HELP file is ambiguous unknown More information available on: Topic ? Sub-Topic ? Sub-Topic ?#FMT(A) Sub-Topic ?Topic ?#FMT(A) ? PARKHELP ERROR:: keyword too long...truncating to 30 charactersEMERGENCY STOP:: Buffer overflow in ARK_HELP#FMT3(I5)#FMT3(I5)#FMT3(I5)#FMT3(I5)Type for more...#FMT(A) (A) (A) Park_help.f(I5)(I5)(I5)(I5)(A) /SEQUENTIALUNFORMATTEDAPPENDREADONLYOVERWRITENEWOVERWRITEUNKNOWNTAPEDIRECT:~/$ ARKTESTARKHELPARKDATA#FMT/( ERROR:: Cannot expand other user's home( ' ERROR:: Cannot expand other user''s home' )#FMT *$ ERROR:: UNIX file name syntax error( ' ERROR:: UNIX file name syntax error' )HOME #FMT,& ERROR:: Non-existent environment name( ' ERROR:: Non-existent environment name' )#FMT.( ERROR:: Running out of file name buffer( ' ERROR:: Running out of file name buffer' )/#FMT(a)#FMT(a)ERROR writing to log file, closing log#FMT(a)Log file already openSEQUENTIALFORMATTEDAPPENDNEWlog ERROR:: failed to open the log file#FMT  ( a, ' ', $ ) . sys.f120( ' ERROR:: Cannot expand other user''s home' )125( ' ERROR:: UNIX file name syntax error' )130( ' ERROR:: Non-existent environment name' )140( ' ERROR:: Running out of file name buffer' )(a) (a) (a) 100( a, ' ', $ ) azAZgetlun.f00<0H0T0`0l0x00000000000000 0,080D0P0\0h0t0000000000000~0{0x(0u40r@0oL0lX0id0fp0c|0`0]0Z0W0T0Q0N0K0H0E0B0? 0<09$06003<00eeffff-f=fMf]efmf}ee  ffZ f ojoo<0$ ooTPIMMS > MODEL FROM INSTRUMENT TO GO SHOW DIRECTORY LOG OUTPUT QUIT EXIT $ASCDS_PROP_PMS_DATA $ASCDS_PROP_PMS_MODEL $ASCDS_PROP_PMS_DATA 44U4q44$ASCDS_PROP_PMS_MODEL $ASCDS_PROP_PMS_MODEL `dblackbody bremsstrahlung powerlaw gaussian raymondsmith 4>$ASCDS_PROP_PMS_DATA flux ergs photons mcrab mjansky unabsorbed angstroms density normalization #@GJ$ASCDS_PROP_PMS_DATA FILR$ASCDS_PROP_PMS_MODEL $ASCDS_PROP_PMS_DATA D6F6|6~66666666666$ASCDS_PROP_PMS_MODEL $ASCDS_PROP_PMS_DATA ::<:$ASCDS_PROP_PMS_MODEL 6}tergs/cm/cm/s photons/cm/cm/s mCrab micro-Jansky  =}tD}tJ}tU}t[}tc}th}tz}t~}t}t}tergs/cm/cm/s photons/cm/cm/s mCrab micro-Jansky  }t}t}t}t}t}t}t}t}t}t }t}t}t#}t*}tB}tF}tM}tS}t]}tc}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t}t'}t-}t5}t;}tG}tM}tU}t[}tj}tn}tt}tx}t}t}t}t}t}t}t}t}t$ASCDS_PROP_PMS_DATA ttt"tGtYt|t $ASCDS_PROP_PMS_MODEL &;l?l@!@MNl(nominal)(warm) RlVlZl$ASCDS_PROP_PMS_DATA KO$ASCDS_PROP_PMS_MODEL ?1235679:;=>@AC+-/1:2>=Full Large Small Refreshed Timing ?> 6!Sڴ?w =Vڴ Full FullExtd Large Small Timing Burst BACDzLD?+ ?+ _? =+ 1'?+ ڴ=\)< =Q>z=&(LNRTXZ^`?e4@/pg@J˦aM@fzV @?PP#=q@@1P6W`@%?i P@&F@@ l+ R}D`CC3318 keV-1 MeV 18 keV-100 keV100 keV-1 MeV ;$?$K$M$O$X$Z$\$>&O==s=^+=&<=?AC 3-7 / 14-24 keV 8-19/ 24-48.9 keV 20-41/48.9-98.8 keV 42-78/98.8-194.9 keVSUWY^`b]D_DbD}DDDDDDDDE=>hs>?1'?4?]?ȴ?@$@Mp@7L@PAKA AffB ffB33BBCs3B33C LCJ3CYCC3D@D/LDfC3AffBCþLC)LCBffAAA33Aə` @MtffC>?@@d@,? =p ?`bM?`bM?tj~@e@3?O;dZ?tzG{?xtj~?zG{@g @;?tzG{?zG{?tj~?Q?bM?zG{?(\)@#ffffff@2@9?O;dZ?zG{?(\)@#ffffff@2@9?$/?zG{?(\)@#ffffff@2@9@V@333333333333@V@333333333333@V@333333333333@@@@@@@@@@@@@@@@@@STOP HELP ,4Em%+39A,0>BOSlpfKMPm56<?@DEXY%\%_%%%%%%%c%%%%%% %% %<%EEZ0<X   P T 420g2;N\h4q|   * < @ `   % ' 0 .4 =P@ L! 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-h.XAAirjDV8s6JG_p. epic_pileup.fxrs_pileup.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDW8s6Jm_p./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDW8s6Jm_p. xrs_pileup.fint_limit.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDW8s6JG$p./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDW8s6JG\$p. int_limit.fbat_limit.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDX8s6Jm$p./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDX8s6Jm\$p. bat_limit.fdcd_rrang.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDX8s6JGAq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDX8s6JGAq. dcd_rrang.frd_real.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDX8s6JmAq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDX8s6JmAq. rd_real.fsimp32.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDY8s6JGBq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDY8s6JGBq. simp32.fspec.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDY8s6JmBq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDY8s6JmBq. spec.ftranmm.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDY8s6JGCq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDY8s6JGCq. tranmm.ftranuvo.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDZ8s6JmCq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDZ8s6JmCq. tranuvo.fintcom.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDa8s6JGDq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDa8s6JGDq. intcom.fgetcom.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDa8s6JmDq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDa8s6JmDq. getcom.fset_param.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDa8s6JGEq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDa8s6JGEq. set_param.fget_param.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDb8s6JmEq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDb8s6JmEq. get_param.fforce_comm.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDb8s6JGFq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDb8s6JGFq. force_comm.fark_help.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDb8s6JmFq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDb8s6JmFq. ark_help.fcomm_lib.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDc8s6JGGq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDc8s6JGGq. comm_lib.fsys.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDc8s6JmHq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDc8s6JmHq. sys.flentrim.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDd8s6JGIq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDd8s6JGIq. lentrim.fupcase.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDd8s6J2Iq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDd8s6J2Iq. upcase.fgetlun.fV=10.0;DBG_GEN=4.14.30;sn;backend;raw;R=Sun Fortran 95 8.1 2005/01/07;G=.XAAirjDd8s6JWJq./vobs/ASC_OBS_PROP/src/obs/prop/tools/pimms/source/;/opt/SUNWspro_10/SUNWspro/prod/bin/f90 -I. -c -qoption f90comp -h.XAAirjDd8s6JWJq. getlun.f  ;"ZZfo-B00  8B<<  BXX<`HN Tv\PP=TTL a02.j44)2o4 xw P  h )