|
A CCD pileup model developed by John Davis of MIT.
The 1D pileup model can be applied to model the 1D Chandra spectrum
obtained in the imaging mode. It should not be used for Chandra
grating or 2D image data. This model is used for fitting energy
spectra only.
Subsequent use of Powell and Simplex optimization methods is desirable
when fitting data with pileup model.
Several model parameters describe pileup:
n, f and g0: The values of n, f and g0
should remain frozen; The full discussion of these parameters is
presented in Davis (2001).
alpha:
The value of the parameter alpha should be allowed to vary. alpha
parameterizes "grade migration" in the detector, and represents the
probability, per photon count greater than one, that the piled event
is not rejected by the spacecraft software as a "bad
event". Specifically, if n photons are piled together in a single
frame, the probability of them being retained (as a single photon
event with their summed energy) is given by alpha(n-1). In reality,
the alpha parameter should be a photon-energy-dependent and
detector-chip-dependent matrix; for simplicity, the jdpileup model
assumes a constant value.
ftime:
The ftime and parameter should be set to the value
given in the header keyword EXPTIME of the event file. (Note that
EXPTIME is used instead of TIMEDEL because the latter includes the
transfer time, which ftime should not.)
fracexp:
The fracexp parameter should be set to the
value given in the header keyword FRACEXPO of the ARF file:
JDPILEUP Parameters
1 | alpha | grade migration; probability of a good grade when two photons pile together |
2 | g0 | probability of
grade 0 assignment |
3 | f | fraction of flux
falling into the pileup region |
4 | n | number of detection
cells |
5 | ftime | frame time
[seconds] (keyword EXPTIME in the event file) |
6 | fracexp | fractional
exposure that the point source experienced while dithering on the
chip (keyword FRACPROB in the ARF file) |
The pileup model does not work for pileup in dispersed grating
spectra. The model was designed for imaging pileup,
including pileup by the gratings in zeroth order.
For more information, see Event Pileup in Charge Coupled Devices by John E. Davis and the Sherpa thread on Using a Pileup Model.
See "ahelp integrate" for further information about
source model integration.
This example illustrate the setting of the pileup model.
sherpa> DATA spectrum.pi
sherpa> INSTRUMENT = RSP[myinst]("source.rmf", "source.arf")
sherpa> POW[p]
sherpa> SOURCE = p
sherpa> JDPILEUP[jdp]
sherpa> PILEUP = jdp
sherpa> show jdp
jdpileup[jdp] (integrate: off)
Param Type Value Min Max Units
----- ---- ----- --- --- -----
1 alpha thawed 0.5 0 1
2 g0 frozen 1 1e-120 1
3 f thawed 0.95 0.9 1
4 n frozen 1 1e-120 100
5 ftime frozen 3.241 1e-120 5 sec
6fracexp frozen 0.987 0 1
sherpa> fit
In this example, data is input and a power-law
model component is established and
then defined as the source model for fitting. The command
JDPILEUP[jdp]
establishes the
JDPILEUP model component and assigns it the name
jdp.
The command
PILEUP = jdp then defines this pileup model for use in fitting.
After fitting, display the pileup fractions with SHOW PILEUP:
sherpa> SHOW PILEUP
1: 0.224696 0.541445
2: 0.263513 0.304025
3: 0.206024 0.113808
4: 0.120808 0.031952
5: 0.0566711 0.00717652
6: 0.0221538 0.00134322
7: 0.00742312 0.000215494
8: 0.00217637 3.02503e-05
9: 0.000567189 3.77462e-06
10: 0.000133035 4.23895e-07
*** pileup fraction: 0.458555
Each row represents the number of photons per CCD frame.
The maximum number of rows is 20; here, there were no more than
10 photons piled together per frame.
The left column represents the percentage of frames with
the stated number of photons: here,
22.47% of frames contained a single photon, 26.35% contained
two photons piled together, etc. The right
column indicates the percentage of observed counts with
the stated number of photons: here,
54.14% of recorded counts were comprised of one photon,
etc.. The total pileup fraction is the sum
of the right column, excluding the first row: here, 45.85%
of observed counts actually contain two or more photons piled
together.
- sherpa
-
atten,
bbody,
bbodyfreq,
beta1d,
beta2d,
box1d,
box2d,
bpl1d,
const1d,
const2d,
cos,
delta1d,
delta2d,
dered,
devaucouleurs,
edge,
erf,
erfc,
farf,
farf2d,
fpsf,
fpsf1d,
frmf,
gauss1d,
gauss2d,
gridmodel,
hubble,
linebroad,
lorentz1d,
lorentz2d,
models,
nbeta,
ngauss1d,
poisson,
polynom1d,
polynom2d,
powlaw1d,
ptsrc1d,
ptsrc2d,
rsp,
rsp2d,
schechter,
shexp,
shexp10,
shlog10,
shloge,
sin,
sqrt,
stephi1d,
steplo1d,
tan,
tpsf,
tpsf1d,
usermodel,
xs,
xsabsori,
xsacisabs,
xsapec,
xsbapec,
xsbbody,
xsbbodyrad,
xsbexrav,
xsbexriv,
xsbknpower,
xsbmc,
xsbremss,
xsbvapec,
xsc6mekl,
xsc6pmekl,
xsc6pvmkl,
xsc6vmekl,
xscabs,
xscemekl,
xscevmkl,
xscflow,
xscompbb,
xscompls,
xscompst,
xscomptt,
xsconstant,
xscutoffpl,
xscyclabs,
xsdisk,
xsdiskbb,
xsdiskline,
xsdiskm,
xsdisko,
xsdiskpn,
xsdust,
xsedge,
xsequil,
xsexpabs,
xsexpdec,
xsexpfac,
xsgabs,
xsgaussian,
xsgnei,
xsgrad,
xsgrbm,
xshighecut,
xshrefl,
xslaor,
xslorentz,
xsmeka,
xsmekal,
xsmkcflow,
xsnei,
xsnotch,
xsnpshock,
xsnsa,
xsnteea,
xspcfabs,
xspegpwrlw,
xspexrav,
xspexriv,
xsphabs,
xsplabs,
xsplcabs,
xsposm,
xspowerlaw,
xspshock,
xspwab,
xsraymond,
xsredden,
xsredge,
xsrefsch,
xssedov,
xssmedge,
xsspline,
xssrcut,
xssresc,
xssssice,
xsstep,
xstbabs,
xstbgrain,
xstbvarabs,
xsuvred,
xsvapec,
xsvarabs,
xsvbremss,
xsvequil,
xsvgnei,
xsvmcflow,
xsvmeka,
xsvmekal,
xsvnei,
xsvnpshock,
xsvphabs,
xsvpshock,
xsvraymond,
xsvsedov,
xswabs,
xswndabs,
xsxion,
xszbbody,
xszbremss,
xszedge,
xszgauss,
xszhighect,
xszpcfabs,
xszphabs,
xszpowerlw,
xsztbabs,
xszvarabs,
xszvfeabs,
xszvphabs,
xszwabs,
xszwndabs
- slang
-
usermodel
|