Examining the Uniformity C-K
edge Across the ACIS Detector
There were two observations of 3C 273 taken less than 2 days
apart using the LETG with ACIS where the SIM was shifted by 0 mm
(obs ID 2471) or -8 mm (obs ID 2464). Previously, these observations
were fit independently to spectral models with 5 source-specific
parameters (NH and 2 PL components with
a normalization and photon index, Gamma, each) and several
instrument-specific parameter characterizing the absorption due
to the contaminant. The previous results gave consistent opacities
at the C-K edge but the uncertainties were rather large due to the
presence of many degrees of freedom.
For this analysis, all source spectral shape parameters were held
fixed due to the lack of significant differences between the two
observations. The parameters are Gamma1 = 2.55, Gamma2 = 1.35, N_H
= 1.68e20, and A1 = A2 = A. This commonality is not too surprising
for 3C 273 -- most variations are small over 2 days. Furthermore,
the absorption model was fixed except for a factor t that gives the
optical depth of the contaminant relative to the value predicted
by the model of the
time dependence
for the median date of about 2001.45. The figures show the fits.

Fig. 1: Fit to the LETG ACIS spectrum of 3C 273 taken in June 2001 at
a SIM Z offset of zero. The NH is fixed and other spectral parameters
are fixed, as described above. The contamination factor gives the
optical depth of the contaminant relative to the value expected
from the time dependence model. The jump near 0.5 keV is due to
a systematic error in BI QEs relative to FI QEs that has not yet
been determined at the 10% level.

Fig. 2: Same as Fig. 1 but for the observation obtained at a SIM Z
position of -8 mm. The optical depth due to the contaminant is
slightly larger than in the center of the detector (SIM Z = 0
mm, Fig. 1).
Adjusting the uncertainties for the resultant chisq values
(1.45 and 1.36), t increases from 0.928 +/- 0.027 to 1.063 +/- 0.024
by shifting -8 mm. The chisq values are very close to those obtained
from full 5 parameter models, so there appears to be very little
intrinsic spectral shape change, as required for this test. The ratio
of the values of t is 1.145 +/- 0.042, a 3.5 sigma difference from 1.00,
indicating a significant increase in absorption from the row 512 to row 180.
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Herman Marshall
hermanm@space.mit.edu
Last updated July 7, 2003