ACIS Calibration Information
This page contains current and historical documents regarding calibration of Chandra's Advanced CCD Imaging Spectrometer (ACIS). Items are organized by topic (see menu on left) and are ordered by date for each topic, with most recent items at the top. For topics with on-going monitoring or calibration (e.g. background, gain correction) the status is summarized at the top of the section. Please see also these additional resources:
Background
- Status Blank sky datasets and ACIS "stowed" datasets are available in the CALDB.
- Old blank sky datasets and "stowed" datasets and tools for modeling the quiescent background, created by Maxim Markevitch, can be found at Maxim's ACIS background page. [Apr 2009; deprecated]
- New Background Rates [updated 2023 Oct]:
- Total telemetered background rates (including all grades
and the upper event cutoff at 15 keV) for chips S2
(FI) and S3 (BI) as a function of time. Vertical dashed lines
are year boundaries. Data are plotted through late-August 2017.
Beginning in Cycle 11 (late 2009) the default high energy limit
was changed from 15 keV to 13 keV.
Subsequent 15 keV rate estimates were scaled from 13 keV rates using
13 kev/15 keV conversion factors of 0.82 for S2 and and 0.68 for S3.
These factors were determined from observations (April-July 2009)
when the rates were fairly constant, and with the onboard high
energy limit set to either 15 keV or to 13 keV.
[Click on the figure for a PDF version.]
- Typical total quiescent background rates (cts/s/chip; 2019, averaged April through early October),
including all grades that are telemetered (not just standard
ASCA grades), by chip type and upper energy cutoff.
These values can be used to estimate the probability of telemetry
saturation. Note that the rates have been increasing rapidly in 2016; users should
take into account the likelihood of further increases during this cycle.
Beginning in Cycle 11 (late 2009) the default high energy limit
was changed from 15 keV to 13 keV.
Subsequent 15 keV rate estimates were scaled from 13 keV rates using
13 kev/15 keV conversion factors of 0.82 for S2 and and 0.68 for S3.
These factors were determined from observations (April-July 2009)
when the rates were fairly constant, and with the onboard high
energy limit set to either 15 keV or to 13 keV.
Period (keV) |
Aug 1999 |
2000-2003 |
2009 |
2023 (January - mid October) |
Upper E cutoff |
15 keV |
15 keV |
15 keV |
15 keV† |
13 keV |
12 keV |
10 keV |
Chip S2 (FI) |
10 |
6.3 |
10.7 |
5.4 |
4.5 |
4.4 |
4.0 |
Chip S3 (BI) |
11 |
7.7 |
14.7 |
8.9 |
6.0 |
5.5 |
4.0 |
†Scaled from 13 keV rates
- Approximate on-orbit standard grade background counting
rates (2019, averaged July to mid-September).
The rates are cts/s/chip,
using only ASCA grades 02346, no VF filtering,
excluding background flares and bad
pixels/columns and celestial sources identifiable by eye.
These values can be used for sensitivity calculations
Energy Band (keV) |
I0 |
I1 |
I2 |
I3 |
S1 |
S2 |
S3 |
S4 |
0.3-10.0 |
0.35 |
0.36 |
0.35 |
0.39 |
1.93 |
0.37 |
1.00 |
0.36 |
0.5-2.0 |
0.06 |
0.06 |
0.06 |
0.07 |
0.17 |
0.07 |
0.14 |
0.08 |
0.5-7.0 |
0.17 |
0.20 |
0.20 |
0.23 |
0.52 |
0.21 |
0.63 |
0.19 |
5.0-10.0 |
0.19 |
0.20 |
0.18 |
0.21 |
1.40 |
0.20 |
0.63 |
0.19 |
10.0-12.0 |
0.12 |
0.12 |
0.11 |
0.12 |
1.10 |
0.12 |
0.79 |
0.12 |
- Memos and papers:
-
Chandra ACIS detector background uniformity from ACIS "stowed" backgrounds
T. Gaetz, 24 Feb 2014
-
Particle background observations: dark Moon and ACIS stowed
(PDF) M. Markevitch, 27 Dec 2005
-
Chandra Spectra of the Soft X-Ray Diffuse Background
(PDF), M. Markevitch, et al., 2003, ApJ 583, 70
-
Reducing ACIS quiescent background using Very Faint mode,
A. Vikhlinin, 22 Oct 2002
-
Using Chandra Level 0 Event Histogram Files to Characterize the High-Energy Particle Background
(PDF), B. Biller, P. Plucinsky & R. Edgar, 22 Jan 2002
-
The Temporal Characteristics of the Chandra X-ray Observatory High Energy Particle Background
(PDF), C.E. Grant, M.W. Bautz & S.N. Virani, 2002, ASP Conference Proceedings, 262, 401
-
General discussion of the quiescent and flare components of the ACIS background,
M. Markevitch, 28 Sep 2001
-
ACIS background measurement prior to opening the mirror cover
(PDF), F. Baganoff, 1 Sep 1999
Bias
CC Mode Calibration
Cross Calibration
- Papers:
-
- New SNR 1E0102.2-7219 as an X-ray Calibration Standard in the 0.5-1.0 keV Bandpass and Its Application to the CCD Instruments aboard Chandra, Suzaku, Swift and XMM-Newton (PDF), Paul P. Plucinsky, Andrew P. Beardmore, Adam Foster, Frank Haberl, Eric D. Miller, A.M.T. Pollock, and Steve Sembay, SPIE, 2016
- Cross-calibration of the X-ray Instruments onboard the Chandra, INTEGRAL, RXTE, Suzaku, Swift, and XMM-Newton Observatories using G21.5-0.9, Tsujimoto et al, 2010 (A&A preprint)
- Cross-calibrating X-ray detectors with clusters of galaxies: an IACHEC study, Nevalainen et al, 2010 (A&A preprint)
- The SMC SNR 1E0102.2-7219 as a Calibration Standard for X-ray Astronomy in the 0.3-2.5 keV Bandpass (PDF), Paul P. Plucinsky, Frank Haberl, Daniel Dewey, Andrew P. Beardmore, Joseph M. DePasquale, Olivier Godet, Victoria Grinberg, Eric D. Miller, A.M.T. Pollock, Steve Sembay, Randall K. Smith, SPIE, 2008
Charge Transfer Inefficiency (CTI)
- Status The GRADED mode CTI correction and temperature-dependent CTI correction are included in acis_process_events as of CIAO 4.3. [Dec 2010]
- ACIS CTI @ -120C: Monitoring and analysis of ACIS CTI by the instrument team, C. Grant, updated monthly
- Memos and papers
- Approximate correction for parallel CTI in GRADED mode data (PDF), A. Vikhlinin, CXC Memo, 19 March 2007
- Temperature dependence of charge transfer inefficiency in Chandra X-ray CCDs (PDF), C. Grant, M. Bautz, S. Kissel, B. LaMarr & G. Prigozhin, SPIE, 2006
- Long-term trends in radiation damage of Chandra x-ray CCDs (PDF), C. Grant, M. Bautz, S. Kissel, B. LaMarr & G. Prigozhin, SPIE, 2005
- A charge transfer inefficiency correction model for the Chandra Advanced CCD Imaging Spectrometer (PDF), C. Grant, M. Bautz, S. Kissel & B. LaMarr, SPIE, 2004
- Modeling Charge Transfer Inefficiency in the Chandra Advanced CCD Imaging Spectrometer (PDF), L. Townsley, P. Broos, J. Nousek & G. Garmire, NIMPA, 2002
- Mitigating Charge Transfer Inefficiency in the Chandra X-ray Observeratory Advanced CCD Imaging Spectrometer (PDF), L. Townsley, P. Broos, G. Garmire & J. Nousek, ApJ, 2000
- CTI-Induced Quantum Efficiency Loss in ACIS Front Illuminated Devices [5 Apr 2000]
Detector Geometry
Energy Resolution
Event Grades
Gain
-
The ACIS gain is calibrated by co-adding data from the external calibration source (ECS).
Prior to 2017, time-dependent gain correction files were released in the CALDB every 3 months.
Due to the continued fading of the ECS, which is composed of a 55Fe source with a
half-life of 2.7 years, the ECS data must be co-added over 6 month to
acquire sufficent photon statistics. Since the beginning of 2017, time-depdent
gain correction files are released in 6 month intervals in the CALDB.
- Status We continue to produce time-dependent gain corrections (TGAIN). The gain epochs are now 6 months.
- ACIS gain @ -120 C: Monitoring and analysis for the ACIS gain by the instrument team, C. Grant, updated monthly
Hot/Bad Pixels
Miscellaneous
FEP0 Problem
- Status There has not been a recurrence of the FEP0 anomaly in ~10 years. [Dec 2010]
Ground Calibration
Transfer Streak Calibration
Optical Blocking Filter and Contamination
- Status An updated contamination model (N0007) is included in CALDB 4.4.10. [Jun 2012]
- Memos and papers
- Update to the ACIS Contamination Model [8 Jan 2010]
- ECS line fluxes and illumination pattern from the Ball dataset (PDF), A. Vikhlinin [18 Feb 2009]
- Contamination on the ACIS OBF and Changes in the Low Energy QE [7 Dec 2004]
- Spatial structure in the ACIS OBF contamination (PDF), A. Vikhlinin [9 May 2004]
- Verifying the ACIS Contamination Model with 1E0102.2-7219 (PDF), J. DePasquale, P. Plucinsky, A. Vikhlinin, H. Marshall, N. Schulz & R. Edgar, SPIE, 2004
- Composition of the Chandra ACIS contaminant (PDF), H. Marshall, A. Tennant, C. Grant, A. Hitchcock, S. O'Dell & P. Plucinsky, SPIE, 2003
- In-Flight Optical Blocking Filter Transmission [10 March 2000]
Pileup
Spatial Resolution, Encircled Energy and PSF
Quantum Efficiency and QE Uniformity
Response Matrices
Subpixel Event Repositioning
- Papers
-
- ACIS Sub-pixel Resolution: Improvement in Point Source Detection (PDF), Anderson C S, Mossman A E, Kim D-W, Allen G E, Glotfelty K J & Fabbiano G, 2010, ADASS XX conference series
- Chandra ACIS Subpixel Event Repositioning: Further Refinements and Comparison between Backside- and Frontside-illuminated X-Ray CCDs (PDF), Li J, Kastner J, Prigozhin G, Schulz N, Feigelson E & Getman K, 2004, ApJ, 610, 1204
- Refining Chandra/ACIS Subpixel Event Repositioning Using a Backside-illuminated CCD Model (PDF), Li J, Kastner J, Prigozhin G & Schulz N, 2003, ApJ, 590, 586
- Improvement of the Spatial Resolution of the ACIS Using Split-Pixel Events (PDF), Tsunemi H, Mori K, Miyata E, Baluta C, Burrows D, Garmire G & Chartas G, 2001, ApJ, 554, 496
- Measurement of the subpixel structure of AXAF CCD's (PDF), Pivovaroff M, Jones S, Bautz M, Kissel S, Prigozhin G, Ricker G, Tsunemi H & Miyata E, 1998, IEEE Transactions on Nuclear Science, vol.45, No.2, pp. 164-175
Comments to cxccal (at) cfa.harvard.edu