|
Top
> Suzaku
> Data Analysis
> HXD
> HXD NXB
HXD PIN Background
Summay table of the recommended background
2007.02.26 by the HXD team
*:
FITS header keyword to distinguish the background modeling methods.
**:
FITS header keyword to distinguish the minor revisions of the same model.
2007.02.01 by the HXD team
Dear Suzaku users,
As described in
Suzaku memo 2006-42, the reproducibility of the current
PIN background model becomes significantly worse during
the period of 2006 March-May, probably due to the operational
change of the lower discrimination level of HXD-GSO
(see HXD event log page).
Since the discrepancy (~5%) between the background model and
actual night earth data implies the "over-subtraction"
during the source observation, this will significantly
affects the scientific result, especially in case of
faint sources.
Although the HXD team has been extensively working to improve
the reproducibility, it is difficult to immediately release
a complete new set of background data, due to the
"epoch fragmentation" caused by the high-voltage operations
and long-term degradations of the PIN diodes.
Therefore, to temporarily solve this situation, we release
an development version of the PIN background, only for observations
which suffer from the low GSO-LD level effect.
Please note that these files are
not dead-time corrected, differntly from the current
background, and you need to correct the dead time exactly
in the same manner as that for the cleaned event files.
The new background files
can be obtained from
this page.
The reproducibility of them is still under investigation,
but will be soon reported as an appendix of Suzaku memo 2006-42.
To distinguish new background files from old ones, you should
check the "METHOD" keyword in the FITS header as follows:
unix% fkeyprint aeXXXX_hxd_pinbgd.evt.gz METHOD
This results METHOD = "LCFIT (bgd_d)" for new files,
while it should be METHOD = "PINUDLC" for old ones.
2007.01.24 by the HXD team
We have summarized the method and reproducibility of the
PIN background modeling in the following two documents:
Suzaku memo 2007-01
"The Method of the HXD-PIN Non X-ray Background Modeling"
Suzaku memo 2006-42
"Reproducibility of the HXD-PIN Non X-ray Background"
2006.11.29 by the HXD team
Dear Suzaku users,
As noticed on the
"HXD event log" page
, on 2006 May 24,
bias voltages for 16 out of 64 PIN diodes were reduced from 500 V
to 400 V, to suppress the rapid increase of noise events, possibly
caused by the in-orbit radiation damage. Since the thickness of
depletion layer depends on the bias, this change slightly affected
the energy response of the 16 PIN diodes especially at higher energy
band than 20 keV. The comparison of Crab spectra obtained before
and after the voltage reduction is shown below (see also
the PDF version), in which filled
circles (labeled "W0") indicate data from the 16 PIN diodes while
open circles ("W123") denote spectra from other 48 diodes.
While the effective area stayed almost the same below 15 keV,
it decreased about 10% above 20 keV which corresponds to a few
percent decline of the "total" effective area of HXD-PIN.
In the current PIN response matrices (ver.20060814), this effect is
not yet implemented. In addition, the level and shape of PIN-NXB
are also expected to be different between two bias voltages,
as a consequence of the loss of effective area.
Therefore, especially in case of the faint source observations,
the "standard" PIN analysis, which treat all the 64 diodes with
no distinction, might draw an improper conclusion.
Until the calibration progress solves this situation, the HXD team
temporarily recommend the observers to exclude data from the
"diodes biased with 400 V", and to use the corresponding modified
response matrices,
together with the PIN-NXB event files for the
W123-only analysis. A column named "UNITID" in the PIN event files
is available to select the specified PIN diodes. There are 16 well-type
phoswich units in the HXD and each of them consists of four PIN diodes,
thus the UNITID ranges from 0 to 15, and the units biased with 400 V
corresponds "UNITID=0,1,2,3". Therefore, the condition of "UNITID>3"
should be applied with the "fselect" as follows (XXXX is your sequence ID):
unix% fselect aeXXXXhxd_0_pinno_cl.evt aeXXXXhxd_0_pinno_w123.evt 'UNITID>3'
Please note that you MUST NOT extract W123 data from "the background
for 64 PIN diodes", since the UNITID column is meaningless in the
background event files. Instead of extracting, you have to download
and use another background files from this page.
The current reproducibility of the PIN background is
described in this document (Suzaku memo 2006-42).
On 2006 October 3, another PIN high-voltage was also changed from
500 to 400 V, and the observational data after this date contain
32 PIN diodes biased with 400 V, and the other 32 diodes biased
with 500 V. In these cases, the 'UNITID>7' condition should be applied,
and the response matrices and background files for "W23-only analysis"
should be used. The response matrices are listed here.
The background files can be obtained from this page.
2006.10.12 by the HXD team
These files are "background HXD-PIN event files" prepared by the
HXD team. If you need urgent help, please contact the suzaku help web
site.
General Notes:
- The event rate of BGD event file is 10 times as high as the real
so that the poisson error can be ignored. Therefore, users should
change the exposure of derived spectra and light curve by yourself, by
using fmodhead, and so on.
- The BGD event files have the extension of GTI. The background
estimation is performed inside the GTI. If you filter the
data with your GTI, you should make a new GTI by ANDing
the two GTIs.
- You should correct the dead time of the observation
spectral file to apply the background file correctly.
On the other hand, there is no need to correct dead times for
estimated PIN BGD files. The dead time correction tool (hxddtcor) is
included in the latest version of the Suzaku ftools.
- The BGD event file does not include the CXB. Since the CXB flux is
about 5% of BGD for PIN, you should take it into account after
subtracting the BGD. We will provide the simulated CXB spectrum for the
HXD PIN, but please keep in mind that it is yet to be
confirmed using actual observational data.
- The accuracy of model is
expected to reach as good as 5-10 % of the averaged background.
However, since May 24, 2006, one of four high voltages has been reduced
to 400 V from the nominal bias of 500 V, due to the in-orbit degradation,
and this effect on the detector background has not yet been taken
into account. Guest observers are strongly recommended to verify the
reliability of background, by comparing the model spectrum with
the "earth occultated spectrum" which can be obtained on the condition
of "ELV<-5".
- The BGD modeling is still under development, and the
evaluation of the systematic errors of this BGD event files
has not been done yet. Users should compare
light curves of the observation and the BGD model.
We also encourage users
to compare the earth occultation data of your data that of BGD
event files, to examine the accuracy of BGD model for your data.
Please find a PIN BGD event file for your observation from this page.
The name of the directory means the sequence number of the observation.
Note on PIN CXB
The HXD-PIN BGD event files do not contain the CXB component,
and thus you should estimate it by yourself. One method is to
estimate the CXB level by using the response for the flat
emission distribution. This response file prepared by the HXD team is
available from the link below. This response assumes that the uniform
emission is from the region of 2 deg x 2 deg.
Typical CXB spectrum is reported as follows, based on the HEAO-1
(Boldt 1987 IAUS..124..611B)
9.0e-9 * (E/3keV)**(-0.29) * exp(-E/40keV) erg/cm2/s/str/keV
Everyone should notice that the level and scatter of CXB level is
one of important sciences and thus we cannot say how much level is
correct.
If you have any questions, please contact
Suzaku Help Desk.
ISAS/JAXA Department of High Energy Astrophysics

Last Modified: Thursday, 08-Nov-2007 15:14:01 JST
|