STScI Logo

calnica stsdas.hst_calib.nicmos


NAME · USAGE · PARAMETERS · DESCRIPTION_ · CALIBRATION_KEYWORDS
CALIBRATION_STEPS · EXAMPLES_ · REVISIONS · BUGS · REFERENCES
SEE_ALSO

NAME

calnica -- Apply instrumental calibrations to NICMOS data.

USAGE

calnica input output

PARAMETERS

input [file name]
The name of the input NICMOS data file. Can be either a root name, in which case a "_raw" suffix and ".fits" or ".fit" extension is assumed, or a complete file name.
output [file name]
The name of the output NICMOS data file. If no value is specified for this parameter, output will default to the rootname of the file passed to input.
(crthresh = 4.0) [real, min=0]
Cosmic ray rejection threshold, in units of sigma, to be used in the CRIDCALC step.
(zsthresh = 5.0) [real, min=0]
Zero-read signal detection threshold, in units of sigma, to be used in the ZSIGCORR step.
(barthresh = 3.0) [real, min=0]
Bar detection threshold, in units of sigma, to be used in the BARSCORR step.
(samprej = 0) [int, min=0, max=NSAMP]
Number of initial samples (readouts) to reject in CRIDCALC step.
(writedark = no) [boolean]
Write out dynamically-generated DARK file?

DESCRIPTION

The CALNICA task performs the routine instrumental calibration of NICMOS data, including dark current subtraction, correction for detector non-linearity, flat fielding, conversion to countrates, and cosmic ray identification and rejection.

INPUT AND OUTPUT FILES

The input to the task is usually a file containing the raw data from a NICMOS observation (usually the file with a "_raw.fits" suffix and extension names) and the output is a file containing the calibrated data. All observing modes produce at least one output file from CALNICA, which is a fully-calibrated final image, usually contained in a file with a "_cal.fits" suffix and extension name. MultiAccum mode, however, produces an additional output file, containing intermediate results of processing, usually with a "_ima.fits" file name suffix and extension. The "ima" file contains the fully-calibrated images produced by each of the multiple detector readouts of a MultiAccum observation, while the "cal" file contains a single image that is the result of combining the calibrated data from all readouts.

The input NICMOS images are contained in Image extensions in FITS files, with a set of five extensions for each image: science (EXTNAME=SCI), error (ERR), data quality (DQ), number of samples (SAMP), and integration time (TIME). Input raw data files for MultiAccum observing mode will contain multiple image sets (or "imsets"), one for each detector readout. The intermediate MultiAccum ("ima") files will contain the same number of imsets as the raw data file. The output "cal" file for all observing modes will contain only one imset.

CALIBRATION SWITCHES

The task is completely data driven, in that the calibration steps carried out by CALNICA are determined by the values of certain keywords contained in the header of the file being processed. A list of the calibration keywords, known as calibration "switches", and their functions is shown below. The calibration switches may be edited with the chcalpar task in order to selectively turn on or off desired calibration steps. The hedit task in the images package or eheader in the toolbox.headers package may also be used to change keyword values. The calibration switches may be set to values of "PERFORM" or "OMIT".

WARNING: The calibration switch keywords reside only in the primary header of NICMOS FITS files, therefore it is critically important to specify extension number zero when passing file names to tasks like chcalpar, hedit, and eheader when you want to modify these keywords. For example, to modify calibration keywords in the file n3xe01bhm_raw.fits, be sure to use the file name "n3xe01bhm_raw.fits[0]" as input to these tasks. If you specify an extension other than zero, the keywords you modify will get written into one of the extension headers, where CALNICA will NOT find them.

The NICMOS science file headers also contain a set of keywords known as calibration "indicators". These keywords duplicate the list of calibration switches and indicate to the user whether or not a given calibration step has already been performed on the data contained in a given file.

REFERENCE FILES

Many of the processing steps require the use of calibration reference files or tables, which contain dark-current and flat-field images and the like. The names of the reference files to be used by each step are also given by keywords in the primary header of the input data file. A list of the reference file keywords and the type of calibration data contained in each file is shown below. Note that the reference file keyword values may contain a directory path (either explicitly or via an environment variable) in addition to the file names.

When an environment variable is used as part of a reference file name (e.g. "nref" in FLATFILE = "nref$h5j1437pn_flt.fits"), there are several points that should be borne in mind. First, the environment variable must be defined in the Unix or VMS shell before logging into IRAF, and the directory name must include the trailing "/", e.g.:

setenv nref /data/reffiles/stdata/

Setting an IRAF environment variable "nref" will simply not work. Also, if the reference files are in the users working directory, nref can be set to "./", rather than editing the header to remove the "nref$" string from each reference file name. Furthermore, note that the file name is specified using IRAF notation rather than Unix, i.e. "nref$h5j1437pn_flt.fits" rather than "$nref/h5j1437pn_flt.fits".

RE-ENTRANT CAPABILITIES

Because the structure and content of the input and output files are identical, the CALNICA task can be used in a re-entrant fashion. In other words, output files that contain data that has only received partial processing can be rerun through CALNICA again in order to execute other calibration steps. For example, it would be possible to process an observation with application of only the dark-current subtraction, examine the results, and then resubmit the dark-subtracted data file to CALNICA to then execute subsequent steps such as linearity correction and flat-fielding. This would of course require turning on and off the appropriate calibration switches for each step as desired before each processing run. Note, however, that certain calibration steps require other steps as a prerequisite. For example, because the flat-field reference data have been dark-subtracted, it is necessary to perform dark subtraction on science observations before applying the flat-field correction. CALNICA is aware of the various dependencies and will not allow the user to perform a given step if all of its required dependencies have not also been performed.

CALIBRATION KEYWORDS

------------------------------------------------------------------
|  Calib.  | Calib.   |  Refer.  |                               |
|  Switch  | Indicator|  File    | Function                      |
-----------------------------------------------------------------|
| ZSIGCORR | ZSIGDONE | several  | Correct for zero read signal  |
| ZOFFCORR | ZOFFDONE |   n/a    | Subtract MultiAccum zero read |
| MASKCORR | MASKDONE | MASKFILE | Mask bad pixels               |
| BIASCORR | BIASDONE |   n/a    | Correct wrapped pixels        |
| NOISCALC | NOISDONE | NOISFILE | Calculate statistical errors  |
| DARKCORR | DARKDONE | DARKFILE | Subtract dark current         |
|          |          | TEMPFILE | Temperature-dependent version |
| NLINCORR | NLINDONE | NLINFILE | Non-linearity correction      |
| BARSCORR | BARSDONE |   n/a    | Correct for electronic "bars" |
| FLATCORR | FLATDONE | FLATFILE | Flat-field correction         |
| UNITCORR | UNITDONE |   n/a    | Convert units to count rates  |
| PHOTCALC | PHOTDONE | PHOTTAB  | Calculate photometric values  |
| CRIDCALC | CRIDDONE |   n/a    | Cosmic-ray identification     |
| BACKCALC | BACKDONE | BACKTAB  | Estimate background           |
| WARNCALC | WARNDONE |   n/a    | Generate user warnings        |
------------------------------------------------------------------

CALIBRATION STEPS

The calibration steps, listed by keyword, are:

ZSIGCORR
This step is controlled by the ZSIGCORR calibration switch, which was added to NICMOS image headers in April of 1998. When processing images that were produced before that time, CALNICA will automatically apply this step to all MultiAccum mode observations if both ZOFFCORR and NLINCORR are also being performed. This step computes an expected number of counts for each pixel in the zeroth readout of a MultiAccum. This information is then used later in the NLINCORR step to estimate the absolute charge in each pixel and the appropriate linearity correction for that charge level. The signal in the zeroth read is estimated by 1) subtracting the zeroth read from the first read, 2) subtracting dark current from the difference image, 3) computing a noise estimate for the difference image, 4) scaling the difference image counts to the effective exposure time of the zeroth read (obtained from the SAMPZERO keyword; approximately 0.203 seconds), 5) resetting to zero all pixels in the difference image that have fewer than zsthresh*err counts. This internal image is then passed to the NLINCORR step. The ZEROSIG DQ flag (value=2048) is set for all pixels with detected signal in the zeroth read. ZSIGCORR also compares the absolute count (DN) level of each pixel in the zeroth and first reads with the "super zero read" science (ZSCI) image in the NLINFILE and flags as saturated any that are above the level of ZSCI by more than the saturation value in the [NODE,2] extension of the NLINFILE. The number of pixels flagged as saturated in the zeroth and first reads is reported. This step uses the MASKFILE, NOISFILE, DARKFILE, and NLINFILE reference files.
ZOFFCORR
Subtract the initial ("zeroth") read image of a MultiAccum-mode observation from all subsequent readouts in the exposure. This step must be performed in order to apply subsequent dark, linearity, flat-field, and units conversions and corrections. The data for the zeroth read are physically stored as the last imset in the MultiAccum data files. The zeroth read image is subtracted from all readouts, including itself, so that the zeroth read science image in the output file will be exactly zero.
MASKCORR
Mask pixels that are known to be permanently defective (i.e. hot or cold). This step uses the static bad pixel mask stored in the MASKFILE. Data quality flag values are copied from the DQ image in the MASKFILE to the DQ image of all imsets in the file being processed.
BIASCORR
Correct pixel values that have wrapped around the dynamic range limit of the on-board Analog-to-Digital Converters (ADC's). In Accum, Bright Object, and Ramp mode observations, the subtraction of the final and initial reads is performed on-board in 16-bit integer arithmetic, therefore it is possible for the difference value for a pixel containing a very bright source to exceed the available range of the calculation. Wrapped pixels will show up with a large negative DN value, usually in the range of -26000 to -32768. The BIASCORR step adds an offset of 65536 DN to correct these wrapped values.
NOISCALC
Statistical errors are computed to initially populate the error (ERR) images in all imsets. The error values are computed from a noise model of the NICMOS detectors, which currently is a simple summation (in quadrature) of the detector read noise and the Poisson noise of the detected signal. The results are expressed as a real number of standard deviations. This step uses the NOISFILE which contains the readout noise for each pixel as the 1 standard deviation noise level in electrons. The readnoise values are stored in the science (SCI) image of the NOISFILE. Data quality (DQ) flags set in the DQ image of the NOISFILE are propagated into the DQ images of all imsets being processed.

In versions 3.3 and later of CALNICA, this step also uses the DARKFILE to estimate and account for the level of "shading" signal when estimating the Poisson noise in the detected counts.

For RAMP-mode data, where the variance of the detected signal from multiple readouts is computed on-board, the calculation of errors is not necessary. In this case, the NOISCALC step simply computes the square-root of the variance data already contained in the ERR images in order to place it on the same basis as the errors computed for other modes.

DARKCORR
Correct for the detector dark current by subtracting a dark current reference image of the same exposure time as the science data being processed. This step uses the DARKFILE reference file which contains a set of dark current images, in units of DN's, for various exposure times. For MultiAccum-mode observations obtained using one of the predefined sample exposure time sequences, a DARKFILE for that particular sample sequence must be used. Error estimates of the dark current, stored in the ERR images of the DARKFILE, are propagated, in quadrature, into the ERR images of all processed imsets. Data quality (DQ) flags set in the DARKFILE are also propagated into the DQ images of all processed imsets.

Starting in April 2002, Version 4 of CALNICA incorporates the dynamic determination of a temperature-dependent dark reference file. This uses the methods described in NICMOS ISR 99-010, and was first implemented as a WWW tool, separate from CALNICA. To use the temperature-dependent dark correction, the TEMPFILE keyword in the primary header must be set to the appropriate _tdd reference file name. If you wish to process your image using a static dark reference file, you can set the TEMPFILE keyword to N/A and the dark reference file named in the DARKFILE keyword will be used. Old NICMOS data (generated or retrieved before May 2002) will not have the TEMPFILE keyword, so it will be necessary to add it to the primary header. If the TEMPFILE keyword is not set to N/A, then CALNICA will attempt to generate and use a temperature-dependent dark file, and the reference file named in the DARKFILE keyword will be ignored.

If you want to see the dynamically-generated dark reference file produced, set the "writedark" task parameter to True. This will create a file that looks like a dark reference file, but with only the groups that were actually generated by CALNICA. The format is very similar to that produced by the Web tool, allowing direct comparison of groups. The name of the dark file written will be the same as the rootname of the data file, with the extension "_drk", so you must make sure that a file of this name does not exist when you run CALNICA, or the program will terminate prematurely.

NLINCORR
Correct the integrated counts in the science data for non-linear response of the NICMOS detectors. At low to intermediate signal levels the detector response deviates in a 2nd-order fashion from the incident flux and is easily correctable. At high signal levels - as saturation sets in - the response becomes highly non-linear and is not correctable to a scientifically useful degree. Therefore the NLINCORR step applies a 2nd-order correction term to pixels with signal values below saturation and applies no correction to pixels in the saturation regime but rather flags them in the DQ image as saturated. Error estimates on the correction applied to non-saturated pixels are propagated into the ERR images of all imsets processed. Data quality (DQ) flags set in the NLINFILE are also propagated into the processed DQ images.
BARSCORR
Added in CALNICA v3.3, this step searches for and flags pairs of image rows or columns that are affected by electronic "bars", which are lines of pixels that are alternately higher and lower in value than their surroundings by a contant DN value. The BARSCORR step searches for this signature in the SCI extension of each imset and flags affected pixels as "Bad pixel detected during calibration" (DQ = 256) in the DQ extensions. For MultiAccum observations, these pixels will be rejected when combined with other imsets in the CRIDCALC step, thus eliminating their effects in the final "cal" image. MultiAccum images that do not have the BARSCORR calibration switch in their primary header will automatically receive this correction.
FLATCORR
Remove pixel-to-pixel sensitivity variations and fine structure by multiplying by the (inverse) flat-field response. This step requires the flat-field reference file FLATFILE. The camera number and filter name of the data being processed must match that of the FLATFILE. Error estimates and DQ flags contained in FLATFILE are propagated into the processed images.
UNITCORR
Convert the data from units of counts (DN's) to count rates (DN's per second). This is accomplished by dividing the SCI and ERR image data by the exposure time values contained in the TIME image extension for each imset.
PHOTCALC
Populate photometric parameter keywords in the image header. The keywords populated are: PHOTMODE, PHOTFLAM, PHOTFNU, PHOTZPT, PHOTPLAM, and PHOTBW. This step requires the PHOTTAB reference table, which contains values for the above 6 keywords appropriate for each NICMOS observing mode. An observing mode is any unique combination of camera and filter. This step does not modify the data in any way, but simply populates the values of the 6 photometric header keywords. The values of PHOTFLAM and PHOTFNU are useful for converting observed count rates to absolute fluxes in units of ergs/sec/cm**2/Angstrom or Jy, respectively.
CRIDCALC
Identify and flag pixels suspected of containing cosmic-ray hits. For MultiAccum mode observations, this step also combines the data from all readouts into a single image. In MultiAccum mode, the data from all readouts is analyzed pixel-by-pixel, computing an error-weighted linear fit to the accumulating counts vs. exposure time, rejecting outliers from the fit using iterative sigma-clipping. Pixel samples identified as outliers are flagged in the DQ images of the intermediate MultiAccum ("ima") file, but the pixel values themselves in the SCI and ERR images of the ima file are unchanged. The result of this operation is stored as a single imset in the output "cal" file, in which the final slope and its uncertainty for each pixel are stored in the SCI and ERR extensions, and the number of unrejected samples and their total exposure time are stored in the SAMP and TIME image extensions. Pixels for which there are no unrejected samples, e.g. permanently hot or cold pixels, will be fit separately.

Users have the option of automatically rejecting some number of initial samples (readouts) for all pixels in MultiAccum observations via the "samprej" task parameter. Note that the value specified by this parameter does NOT include the zeroth-read.

The algorithm is not yet completely defined or implemented for Accum, Bright Object, and Ramp mode observations, therefore the "cal" output file for these modes will still contain CR hits.

BACKCALC
Compute a predicted background (sky plus thermal) signal level, based on models of the zodiacal scattered light and the telescope plus instrument thermal background. This step uses the BACKTAB reference table which contains the background model parameters. Results are written to the BACKEST1, BACKEST2, and BACKEST3 header keywords. The image data are not modified in any way.

This step is not yet implemented.

WARNCALC
Issue warning messages if it appears that the science data may be compromised in any way due to unusual instrumental characteristics or behavior. Various engineering keywords values are analyzed and any anomalous readings are reported.

This step is not yet implemented.

EXAMPLES

1. Perform calibration for observation "n3v701qln". Output file(s) are to have the same root name as the input file.


  ni> calnica n3v701qln ""

2. Calibrate the observation "n3t501c2r" and produce output files with a root name of "ngc3603". Set the cosmic ray rejection threshold to 6.5 sigma.


  ni> calnica n3t501c2r ngc3603 crthresh=6.5

3. Perform additional processing on the data contained in file "irc10216_ima.fits" which was produced by a previous run of calnica. Give the output files a root name of "irc10216b".


  ni> calnica irc10216_ima.fits irc10216b

REVISIONS

Version 4.2
Improved CRIDCALC processing. The sample weightings are now more in line with theoretical values, for example, those in Fixsen et al. (2000), PASP, 112, 1350. The ramp fits are now determined iteratively, with each ramp split into pre- and post- cosmic ray sections that are fit independently. The ramp fitting is now done for pixels which have no "GOOD" samples, resulting in far fewer zeros in the _cal file. The DQ flags must be carefully checked to make sure that pixels with known problems are treated appropriately in subsequent analysis. A new DQ flag, HIGH_CURVATURE, was defined to account for those pixels that appear to have more than 3 cosmic rays up the ramp. Since this is statistically extremely unlikely, the most likely explanation is curvature in the ramp. See the NICMOS ISR "CALNICA Update" (2008).
Version 4.1.1
Fixed an array access error in the ZSIGCORR routine.
Version 4.0
New temperature-dependent dark subtraction. Order of processing changed to execute each calibration step on a given group before going on to the next group. Default "barthresh" parameter set to 3.0.
Version 3.3
New BARSCORR routine and associated task parameter "barthresh" were added. Capability to reject user-selected number of initial samples in CRIDCALC and associated task parameter "samprej" were added. Changed all count-to-countrate conversions to use TIME image data for exposure times, rather than the SAMPTIME keyword value. NOISCALC step was enhanced to estimate and account for "shading" signal when estimating noise in detected signal. NLINCORR step was upgraded from use of 1st-order to 2nd-order correction scheme. Rejection of electronic noise spikes in CRIDCALC step was enhanced.
Version 3.2.2
Modification of internal library interface.
Version 3.2.1
Fixed a memory allocation bug that was causing the task to crash on Linux systems.
Version 3.2
Use of the new ZSIGCORR, ZSIGDONE, and SAMPZERO keywords in the ZSIGCORR step was added. The ZSIGCORR step was also modified to make use of any good data in the zeroth readout for those pixels that are already saturated in the first readout. The CRIDCALC step was also modified to make use of the zeroth read data for these pixels when computing an output value for the "cal" file. Use of the new ZEROSIG and GROT data quality flag values was implemented. CALNICA treats these conditions as warnings only and will not reject any pixels containing only these DQ values. Relaxed the exposure time matching criterion for the dark current reference data to one-tenth of a second. Added computation of output image median statistics for populating the new median statistics keywords GOODMEDN, QAMEDN, QBMEDN, QCMEDN, and QDMEDN.
Version 3.1.2
Modified the routine that writes processing history keywords to the output image headers to correct a bug that was causing the task to crash on HP/UX systems.
Version 3.1.1
Modified the calnica cl script so that it issues the proper command to run the host-level calnica executable on VMS systems. Fixed a bug that was causing the task to crash when processing NSAMP=2 MultiAccum exposures.
Version 3.1
Modified to recognize the new file name suffixes used for the flat field and background images obtained with Target Acquisition observations. The raw file name suffixes are "rwf" and "rwb" (for the flats and backgrounds, respectively), and the corresponding calibrated file name suffixes are "clf" and "clb".
Version 3.0
The wrapped pixel correction threshold in the BIASCORR step was changed from -26000 to -23500 DN. The CRIDCALC routine was rewritten so that it no longer needs the NOISFILE to compute errors and eliminated the huge values that occasionally resulted from rejecting all but 1 sample for a pixel. The order in which MultiAccum readouts are processed was reversed so that the readouts are now processed in chronological order (zeroth readout first, final readout last). Added the use of command-line arguments crthresh and zsthresh so that the user can set rejection thresholds. Added the ZSIGCORR routine which calculates the amount of signal in the zeroth read of a MultiAccum and accounts for that signal when performing NLINCORR.

BUGS

REFERENCES

Authors: Howard Bushouse, Science Software Group, STScI Robert Jedrzejewski, Science Software Group, STScI

The following additional references are available from STScI and the NICMOS instrument group and describe in more detail the NICMOS calibration process and general usage of STSDAS:

	"The STScI NICMOS Pipeline: CALNICA, Single Image Reduction",
		Instrument Science Report NICMOS-028
        "NICMOS Data Handbook"
        "NICMOS Instrument Handbook"
        "STSDAS Users Guide"
        "Phase II Proposal Instructions"

The following are technical references meant for internal usage and are not written as "end-user" products. However, these documents can be retrieved if a detailed understanding of the software is required.

The reference tables and images are controlled by CM. The document describing the contents and form of the reference data is "Post Observation Data Processing System to Calibration Database System Interface Control Document", (ICD-47).

The header keywords found in the data files are controlled by CM. The document describing the keywords is "Post Observation Data Processing System to Space Telescope Science Data Analysis Software Interface Control Document", (ICD-19).

SEE ALSO

eheader, hedit, chcalpar, calnicb


Source Code · Package Help · Search Form · STSDAS