XRCF Source Spectral Analysis
XRCF Source Spectral Analysis
|
June 17, '99 Final Version
Automated analysis results
of HSI-grating data sets.
- HRMA, Grating, HSI calibration files are from CALDB-Cal area,
specific file names are given in the
source code.
- The HSI data are corrected for the
HSI QE depression and
"tile plots" are made to show this effect.
- MARX-compatible modeled source-spectra files
are available
- The source model is via dd's kludgy IDL routines:
xss_sim.pro.
- ( Jan.2 '98 version of these analyses is still available for comparison
here .)
|
- Carbon continuum analysis
and XSPEC fitting
- Some manual analysis of EIPS Targets
- Other Source info
- Other Source Pages
The Al anode produces Al K-alpha, "satellite lines", Al-K beta
as well as contaminating C and O lines.
Name | Energy | Wavelength |
Relative Intensity |
Al K-a | 1.48670 | 8.33961 | 1.0000 |
Al K-a sat | 1.4959 | 8.2883 | 0.125 |
Al K-b | 1.55745 | 7.96077 | 0.017 |
continuum Alx2 | 1.1-1.6 | 7.7-11.2 | 0.076 |
- MEG-HSI +3rd order Al
image and spectrum,
from D-HXH-FC-28.003,
970109, hsi108034i0.fits. Centered in the image is the 3rd order Al K-alpha
line with
the satellite line blend just to its left and K-beta further to left. The
source here has an Alx2 filter in place and the filter cutoff is seen as well.
The Be anode produces a big broad Be K-alpha line,
and probably contaminating C and O lines.
Name | Energy | Wavelength |
Relative Intensity |
Be K-a | 0.10850 | | 1.0000 |
- LETG-HSI spectrum D-LXH-3D-12.004 of the Be anode with Bex2 filter
agrees pretty well (see
comparison in automated analysis) with
a single line having an E/dE_FWHM of 12.
The C anode produces a big broad C K-alpha line,
and probably contaminating O line.
Name | Energy | Wavelength |
Relative Intensity |
C K-a | 0.2774 | | 1.0000 |
- LETG-HSI spectrum D-LXH-3D-11.047 of the C anode with C8H8x2 filter
agrees pretty well (see
comparison in automated analysis) with
a line which is made up of two gaussian components:
one at 1.002 times the C-K energy (with E/dE_FWHM = 30), and one
at 0.965 times the C-K energy (with E/dE_FWHM = 25) and 0.085 times
the area of the first.
Fe-K
Name | Energy | Wavelength |
Relative Intensity |
Fe K alpha | 6.40 | | 1.0000 |
Fe K beta | 7.06 | | 0.002 guess |
The Mg anode produces Mg K-alpha, "satellite lines", Mg-K beta
as well as contaminating C
and O lines.
Name | Energy | Wavelength |
Relative Intensity (all detectors) |
Mg K-a | 1.2536 | | 1.0000 |
Mg K-a sat 1 | 1.2618 | | 0.086 |
Mg K-a sat 2 | 1.2632 | | 0.062 |
Mg K-b | 1.3022 | | 0.01 ? |
continuum ... | | | ? |
- LEG-HSI +5th order Mg(+C+O)
image and
histogram,
from D-LXH-dF-16.001,
970116, hsi109001i2.fits. Centered in the image is the 5th order Mg K-alpha
line with
the satellite lines blended just to its left.
The 1st order C-K line, broad one at left, has
E/dE ~ 30, the 2nd order O-K line has E/dE ~ 120 in its core (see
O-K below, however.)
- HEG-HSI +2nd order Mg histogram,
from D-HXH-dF-16.003,
970116, hsi109003i2.fits. The two satellite lines are resolved
(at energies 1.0065 and 1.0077 from the K-alpha) and the as-observed
E/dE of the K-alpha line is ~1080.
The Mo anode produces Mo L-alpha, beta, Mo M line,
as well as contaminating C and O lines. The HEG-HSI spectrum below suggests
an E/dE of ~300 for the L lines. Two weak lines (2.45 keV and 1.98 keV)
are seen also.
Name | Energy | Wavelength |
Relative Intensity (all detectors) |
Mo L-a | 2.2932 | 5.4066 | 1.0 |
Mo L-b | 2.3948 | 5.1773 | 0.444 |
Mo ? | 2.45 | 5.06 | 0.086 |
Mo ? Ir M? | 1.98 | 6.26 | 0.052 |
continuum | 2.0-2.5 | 4.96-6.2 | 0.116/0.1 keV |
- Mo-Mox2 MEG HSI image and spectrum from
D-HXH-3D-23.034, 970125/hsi110151i0.fits.
- Mo-Mox2 HEG HSI image and spectrum from
D-HXH-3D-23.035, 970125/hsi110154i0.fits.
- Mo-Mox2 HEG HSI histogram with source model over plotted. Additional lines around 2.45 keV (bin 406) and 1.98 keV (bin 650) are
visible above the continuum.
- X-GEF SSD data
gives for Mo La/(La+Lb) ~ 0.72, compared with 1.0/1.444 = 0.693 measured here - pretty
good agreement actually!
The SiO anode, run at ~1.7 keV, produces the O-K line, continuum,
and possibly contaminating C line. The LEG-HSI spectrum and HEG-HSI spectrum
show identical line shape that is well modeled by two broad, E/dE = ~120, lines:
one at 0.5249 keV and one at 0.991*0.5249 keV with relative intensity 1.0:0.3 .
By "O-K" line we mean this whole/combined line profile.
Name | Energy | Wavelength |
Relative Intensity |
O-K | 0.5249 | 23.62 | 1.0 |
local continuum | ~0.5 | | 0.266 / 0.1 keV |
continuum w/CrLx2 | 0.46-0.56 | | 0.25 |
- OK,CrLx2 LEG HSI image and spectrum from
D-LXH-3D-11.042, 970118/hsi109293i0.fits.
- OK,CrLx2 HEG HSI image and spectrum fromD
D-HXH-3D-11.044, 970119/hsi109295i0.fits. The O-K line here is no broader than
as observed with the LEG, indicating that this is the intrinsic line shape.
- Two-gaussian approximation
to the O-K line shape (LEG data).
The Ti anode, run at high voltage, produces Ti K-alpha, Ti-K beta, Ti-L lines continuum and contaminating C and O lines. Used with a TiKx2 filter the continuum may be hard to separate from the K-a K-b lines in FPC spectra.
Name | Energy | Wavelength |
RI@ Source | RI@ BND-FPC |
Ti K-a | 4.51084 | 2.7486 | 1.0000 | 1.0000 |
Ti K-b | 4.93181 | 2.5140 | 0.181 | 0.169 |
Continuum w/filter | 4.-4.9 | 2.5-3.3 | ~0.2 | ~0.2 |
- HEG-HSI +1st order Ti-K lines image and
spectrum,
from E-HXH-3D-10.007,
970203, hsi111121i0.fits. Centered in the image is the 1st order Ti K-alpha
line, K-beta is to left. Measured K-b/K-a ratio here is 0.171 +/- 0.005; the
HRMA-HEG-HSI response at 4.9 relative to 4.5 keV is ~ 0.944 so the source
K-b/K-a ratio is ~0.181. THe BND-FPC relative response K-b/K-a ~0.935 so
BND-FPC ratio is ~0.169.
- Modeled Ti w/TiKx2 spectrum
and what it looks like to a BND-FPC.
See /data/letg1/bnd_rate/phase_one.html for stability plots for the Source-BND .
MIT Accessibility