11.2 Exposure Sequences and Contemporaneous Calibrations
There are several instances when a series of associated STIS exposures (rather than a single exposure) will be taken. The data from these exposure sequences are generally processed as a single unit through the STScI calibration pipeline, with the scientific data from the multiple associated exposures appearing in a single file (for a high-level overview of the STIS calibration pipeline and the data product format see Chapter 15). While you do not have to specify that you plan a series of associated exposures in your Phase
I proposal, it is helpful to know about these sequences when planning your proposal. In Phase
II, once your proposal has been accepted and you are working on scheduling your observations, you will be able to see and use these sequences. All are generated from a single exposure logsheet line in your Phase
We discuss several types of associated exposures below:
- Automatic wavecal exposures taken with scientific data to allow calibration of the spectroscopic and spatial zero points.
CR-SPLITexposures taken to allow removal of cosmic rays in the scientific data during post-observation data processing.
- Multiple identical repeat exposures, which can be taken to provide time resolutions of tens of seconds (CCD) or minutes (MAMA).
- Pattern sequences, in which the target is stepped, for example along the slit to mitigate the impact of hot pixels or perpendicular to the slit to map a two-dimensional region for spectroscopic observations, or in a dither pattern for imaging observations.
In addition, there are two types of contemporaneous calibration observations that observers may take with their scientific observations in special circumstances:
- GO wavecals, taken if exceptional wavelength accuracy is required, or for slitless spectroscopy.
- CCD fringe flats (
CCDFLAT) which need to be taken for near-infrared (NIR; λ > 7500 Å) observations in the grating modes if high signal-to-noise is required.
The STIS optical path from source to detector passes through the aperture (slit) wheel (where the filters for imaging also are housed) and then reflects from one of the elements mounted on the Mode Selection Mechanism (MSM) which houses the first-order gratings, the prism, the cross-dispersers for use with the echelles, and the mirrors for imaging work (see Figure 3.1). Lack of repeatability in the MSM causes the center of the spectrogram (as defined by the aperture and wavelength centers) to fall on a slightly different detector location each time there is a movement of the MSM (the MSM-induced offsets in dispersion and the spatial direction have been measured to be ±3 pixels or less). In addition, for MAMA first order spectrographic observations, the aperture location on the detector is deliberately shifted each month to ensure equalization of extracted charge across the detector.
To allow calibration of the zero point of the aperture location and the zero point of the wavelength scale for spectroscopic observations, a line lamp observation (so-called wavecal) is taken automatically each time the MSM is moved. In addition, if a series of exposures or a single long exposure is taken at a single MSM setting, then an additional wavecal will automatically be taken when there is a pause in data taking if 40 minutes of exposure time has passed since the previous wavecal. Here, 40 minutes is the time constant for thermal changes which might affect the wavelength accuracy. Testing in orbit has shown that in extreme conditions (when there is a swing from hot to cold), worst-case thermal shifts of roughly 0.3 pix/hr can be seen; however, monitoring shows that under typical observing conditions, thermal drifts are of the order of 0.1 pix/hr (see also the Monitoring page on the STIS website).
To summarize, each set of spectroscopic scientific exposures taken at a given grating tilt (i.e., MSM position) will normally be accompanied by at least one automatically taken wavecal exposure. This auto-wavecal will be taken prior to the science exposure. Additional auto-wavecals will be taken at the first pause in data taking after ~2300 seconds of exposure time at that grating position have elapsed. For MAMA observations in particular, auto-wavecals can be forced into occultation by (1) keeping exposures in an orbit at the same grating setting, and implementing either (2a) a single long exposure that fills the visibility period or (2b) shorter exposures whose sum is less than ~2300 seconds since the last auto-wavecal, followed by an exposure that crosses the 2300 second boundary and fills the remainder of the visibility period. Similarly, if spectroscopic drifts are a concern, MAMA observations can be split into exposure sums that are ~2300 seconds in duration to maximize the occurrence of auto-wavecals. Multiple auto-wavecals occur more naturally for CCD observations which are usually CR-split into exposures of ~1000 seconds, or less, in duration.
These wavecal exposures will be processed along with the scientific data, and they will be used by the pipeline to automatically correct the zero-point offsets in the wavelength and spatial scales (see Chapter 15).
The automatic wavecals are designed to be of sufficient duration to produce spectrograms which contain at least 3 emission lines with 3 counts/pix and 50 counts summed over the line. In those regions of the spectrum where 3 lines are not obtainable, there will be at least 1 emission line with 18 counts/pix and 300 counts summed over the line. For the CCD where integration times are short, the auto-wavecals will typically be taken to ensure roughly 8 times this signal.
The combination of thermal changes between the wavecal and scientific exposures, coupled with the ability to measure the zero points in the wavecal exposures, limits the accuracy of the absolute zero points to ≤0.2 pixels (see Section 16.1). In addition to the auto-wavecals, observers can also take their own wavecal exposures, using the
WAVE target option (see GO Wavecals) if they desire more accurate wavelengths than will automatically be provided, or they are particularly concerned about the time variation of the zero point.
The auto-wavecals can be omitted by using the exposure level optional parameter
WAVECAL=NO. Note, however, that using this option on any exposure in a visit will turn off auto-wavecals for all exposures in that visit. The observer will then have to include sufficient GO wavecals to allow adequate wavelength calibration of their data.
Beginning in Cycle 25, the
WAVECAL=NO optional parameter will be included in the supported availability mode. Observers will no longer need approval to disable auto-wavecals to reduce overhead during orbital visibility. Observers will be required to include GO wavecals at each MSM position when using this option.
Only if you require particularly accurate wavelengths do you need to consider using the
TARGET=WAVE option to insert additional wavecal exposures into your observing sequence.
The wavecals taken with
TARGET=WAVE are identical to those taken automatically (i.e., the auto-wavecals) with two important exceptions. First, you can explicitly specify which aperture (slit) you wish to use for the
TARGET=WAVE exposure (whereas for automatic wavecals the program slit or a pre-defined alternative for each grating is used). Second, you can take longer exposures, increasing the signal-to-noise of the lamp exposures or possibly saturating some lines to bring out weaker lines near astronomical lines of interest.
TARGET=WAVE exposures cannot be taken with all slit-grating combinations. In particular, the line lamps can be too bright for the MAMA detectors when used with wide slits. Therefore only certain aperture-grating combinations can be used for
TARGET=WAVE observations. Tables of lines and observed count rates from the line lamp for each grating mode for several different apertures and the complete list of allowed combinations are provided on the GO Wavecal Aperture Selection web page. When entering a GO Wavecal in APT, only the permitted slits will be displayed in the
Although the slit wheel repeatability is very high (see Section Slit and Grating Wheels), observers wishing particularly accurate wavelength calibrations may wish to use a slit for their scientific exposures for which there is an allowed slit-grating wavecal; otherwise, the slit wheel will be moved each time they take a wavecal exposure, producing a small additional uncertainty.
In order to allow rejection of cosmic rays in post-observation data processing, observers using the STIS CCD should always try (as much as possible given signal-to-noise ratio constraints when in the read-noise-limited regime) to obtain at least two—preferably three or more—identical CCD exposures (see Section 7.3.4). In Phase
CR-SPLIT optional parameter (default value 2) allows easy scheduling of such multiple associated exposures. You specify the total exposure time and set
CR-SPLIT=n, where n is the number of exposures to break the total observing time into. For example, if the total exposure time is 12 minutes, and
CR-SPLIT=3, then three 4-minute exposures will be taken. Those three exposures will be associated with one another, passed through the STScI calibration pipeline as a unit, and a cosmic-ray–free image will be produced during pipeline processing (see the "STIS Calibration" Chapter of the STIS Data Handbook). Allowed values of
CR-SPLIT are integers from 1 to 8. Note that overheads are incurred for each
11.2.3 Fringe Flat Fields
The STIS CCD exhibits fringing in the far red, limiting the signal-to-noise achievable at wavelengths longward of ~7500 Å in the
G750M spectral modes. As discussed in Section 7.2.6, the best way of eliminating the fringes in the far red is by obtaining contemporaneous flat fields along with the scientific observations. These "fringe flats" must be taken at the same position of the Mode Selection Mechanism as the scientific data. STIS users can insert such contemporaneous fringe flat fields into the same visits as their scientific data, as described below.
Designing Your Fringe Flat-Field Observations
Observers of extended sources will typically want to take their fringe flat fields using the same slits as they use for their scientific targets, since the flat-field lamp will then illuminate the detector in the most similar way to the targets. However, observers of point sources will typically fare better if they use small slits (e.g., those which are otherwise used for echelle observations) for their fringe flat fields. The main reason for this difference is that the PSF of the STIS CCD features a substantial halo in the far red containing up to 20% of the total source flux, which causes the fringes in lamp flat fields to behave differently from those of external sources, especially in the case of point sources (see also Section 7.2.8). Fringe flat fields taken with short slits simulate the spatial structure of point sources significantly better than those taken with long slits.
The slits supported for scientific observations with the
G750M gratings and the associated slits to use for fringe flat fields in the cases of both extended- and point-source observations in the far red are listed in Table 11.1.
Table 11.1: Slits for Extended-Source and Point Source Fringe Flat Fields.
Fringe Flat Slit for
Fringe Flat Slit1 for
1 Short slits are chosen so as to be concentric with matched long slit.
E2 positions are chosen to be concentric with
52X0.1 aperture at row 900.
A few notes are of importance on the use of short slits for obtaining fringe flat fields:
- Fringe removal for sources that are offset from the center of the long slit will not be possible with a short-slit fringe flat field; one has to use long-slit fringe flat fields for those cases. A special case in this respect is that of point-source spectra with the
52X0.2F1slit, as the
0.3X0.09slit (which is in principle the appropriate one to use for fringe flats in that case, cf. Table 11.1) is only a few CCD pixels larger than the occulting bar of the
52X0.2F1slit. However, a short-slit fringe flat does give a somewhat better fringe correction for the area covered by both the short slit and the
52X0.2F1slit, so if that area is of particular scientific interest, we recommend taking a short-slit fringe flat as well.
- The limited length of the short slits used for obtaining contemporaneous flat fields of point sources (0.2–0.3 arcseconds) does not allow one to sample the full PSF, so that absolute spectrophotometry cannot be performed with the short-slit fringe flat fields alone. However, a comparison with the pipeline-reduced point-source spectrograms will enable a proper flux calibration.
- At wavelengths longward of ~7500, fringing is the dominant calibration concern at high S/N, whereas imperfect charge transfer efficiency (CTE) is the dominant concern at low S/N ratios. We therefore recommend using the
E2pseudo-apertures for faint sources and the normal aperture positions in the long slits for high S/N observations.
E2aperture positions are, like the
E1aperture positions, located near row 900 of the detector, and are intended to be used to mitigate CTE effects. However, in order to better align with the
52X0.1aperture, which is used for fringe flats near row 900, the targeted position is offset about 1 pixel in the dispersion direction from the physical center of each aperture. Fringe-flat alignment will be slightly better than when using the
E1positions, although for the
52X0.2E2aperture, the throughput will be slightly reduced. The
E2positions should only be used for point source observations where fringe flats are needed and CTE is a concern. If a peakup is desired before using the
E2aperture positions, it should be done using the
- The limited length of the short slits used for obtaining contemporaneous flat fields of point sources (0.2–0.3 arcseconds) imposes a minimum requirement on the accuracy of the acquisition of target point sources in the slit. The final accuracy should be of the order of 1 pixel (i.e., ~0.05 arcseconds). In case the observer has to use offset acquisition targets, it is therefore recommended that an
ACQ/PEAKexposure in a short slit be performed to ensure centering in both directions (see Chapter 8).
Inserting Fringe Flat-Field Exposures in Phase
A fringe flat-field exposure is specified in your Phase
II proposal input as follows:
Target_Name = CCDFLATto indicate the exposure as a fringe flat field. The flat-field exposure will automatically be taken at
= 2(to allow cosmic-ray rejection and to obtain adequate signal-to-noise).
Aperturemust be one of
Wavelengthmust be one of the following combinations:
G750Land Wavelength: 7751
G750Mand Wavelength: one of 6768, 7283, 7795, 8311, 8561, 8825, 9286, 9336, 9806, or 9851.
DEF(Default). The default exposure time is determined from in-flight calibration data and ensures a signal-to-noise of 100 to 1 per pixel for all settings mentioned above and
Number_Of_Iterations = 2.
- If the scientific data are taken in binned mode, specify Optional Parameters
BINAXIS2in the same way as for scientific observations. Supported binning factors are 1, 2, and 4.
Two very important issues for fringe flat fields:
- Fringe flat-field exposures are moved into the occulted period whenever they occur as the first or last exposure in an orbit. Thus you can fill the unocculted portion of your orbit with scientific observations and take the fringe flat during the occultation by placing it at the beginning or end of the orbit.
- Fringe flat fields are effective only if taken without a move of the Mode Selection Mechanism between the scientific exposure and the fringe flat field. Observers must ensure that if the spectral element or wavelength setting is changed during an orbit in which they wish to obtain a fringe flat, then they place the fringe flat-field exposure immediately before or after the scientific exposure(s) they wish to de-fringe. In some cases (e.g., for a long series of exposures), the observer may choose to bracket the scientific exposures with fringe flat-field exposures to be able to account for any thermal drifts.
Please refer to the STIS ISR 1997-15 for more details about NIR fringe flats; STIS ISR 1997-16 which deals with fringing in spectrograms of extended sources; STIS ISR 1998-19 (Revision A) which deals with fringing in spectrograms of point sources as well as more general fringing analysis and details related to the
52X0.2F1 aperture; and STIS ISR 1998-29 which is a tutorial on the use of IRAF tasks in the stsdas.hst_calib.stis package to remove fringes. Currently, an effort to port these defringing tasks to Python is underway. Once completed, they will be hosted as a part of stistools: https://stistools.readthedocs.io/en/latest/index.html
11.2.4 Repeat Exposures
A series of multiple repeated identical exposures can be taken most easily using the
Number_Of_Iterations optional parameter in Phase
II. In this way, time-resolved observations at minimum time intervals of roughly 20 seconds for the CCD (if subarrays are used) and 30 seconds for the MAMA can be taken in
ACCUM operating mode. The output of this mode is a series of identical exposures. If your exposure time is 60 seconds, and you set
Number_Of_Iterations=20, you will obtain twenty 60-second exposures. These twenty exposures will be associated with one another and processed through the pipeline as a unit—the individual exposures will be fully calibrated and a summed image will also be produced for MAMA data as well as a cosmic-ray rejected image for CCD data (see also Chapter 15).
STIS Instrument Handbook
- • Acknowledgments
- Chapter 1: Introduction
Chapter 2: Special Considerations for Cycle 28
- • 2.1 STIS Repair and Return to Operations
- • 2.2 Summary of STIS Performance Changes Since 2004
- • 2.3 New Capabilities for Cycle 28
- • 2.4 Use of Available-but-Unsupported Capabilities
- • 2.5 Choosing Between COS and STIS
- • 2.6 Scheduling Efficiency and Visit Orbit Limits
- • 2.7 MAMA Scheduling Policies
- • 2.8 Prime and Parallel Observing: MAMA Bright-Object Constraints
- • 2.9 STIS Snapshot Program Policies
- Chapter 3: STIS Capabilities, Design, Operations, and Observations
- Chapter 4: Spectroscopy
- Chapter 5: Imaging
- Chapter 6: Exposure Time Calculations
- Chapter 7: Feasibility and Detector Performance
- Chapter 8: Target Acquisition
- Chapter 9: Overheads and Orbit-Time Determination
- Chapter 10: Summary and Checklist
- Chapter 11: Data Taking
Chapter 12: Special Uses of STIS
- • 12.1 Slitless First-Order Spectroscopy
- • 12.2 Long-Slit Echelle Spectroscopy
- • 12.3 Time-Resolved Observations
- • 12.4 Observing Too-Bright Objects with STIS
- • 12.5 High Signal-to-Noise Ratio Observations
- • 12.6 Improving the Sampling of the Line Spread Function
- • 12.7 Considerations for Observing Planetary Targets
- • 12.8 Special Considerations for Extended Targets
- • 12.9 Parallel Observing with STIS
- • 12.10 Coronagraphic Spectroscopy
- • 12.11 Coronagraphic Imaging - 50CORON
- • 12.12 Spatial Scans with the STIS CCD
Chapter 13: Spectroscopic Reference Material
- • 13.1 Introduction
- • 13.2 Using the Information in this Chapter
- • First-Order Grating G750L
- • First-Order Grating G750M
- • First-Order Grating G430L
- • First-Order Grating G430M
- • First-Order Grating G230LB
- • Comparison of G230LB and G230L
- • First-Order Grating G230MB
- • Comparison of G230MB and G230M
- • First-Order Grating G230L
- • First-Order Grating G230M
- • First-Order Grating G140L
- • First-Order Grating G140M
- • Echelle Grating E230M
- • Echelle Grating E230H
- • Echelle Grating E140M
- • Echelle Grating E140H
- • PRISM
- • PRISM Wavelength Relationship
- • 52X0.05 Aperture
- • 52X0.05E1 and 52X0.05D1 Pseudo-Apertures
- • 52X0.1 Aperture
- • 52X0.1E1 and 52X0.1D1 Pseudo-Apertures
- • 52X0.2 Aperture
- • 52X0.2E1, 52X0.2E2, and 52X0.2D1 Pseudo-Apertures
- • 52X0.5 Aperture
- • 52X0.5E1, 52X0.5E2, and 52X0.5D1 Pseudo-Apertures
- • 52X2 Aperture
- • 52X2E1, 52X2E2, and 52X2D1 Pseudo-Apertures
- • 52X0.2F1 Aperture
- • 0.2X0.06 Aperture
- • 0.2X0.2 Aperture
- • 0.2X0.09 Aperture
- • 6X0.2 Aperture
- • 0.1X0.03 Aperture
- • FP-SPLIT Slits 0.2X0.06FP(A-E) Apertures
- • FP-SPLIT Slits 0.2X0.2FP(A-E) Apertures
- • 31X0.05ND(A-C) Apertures
- • 0.2X0.05ND Aperture
- • 0.3X0.05ND Aperture
- • F25NDQ Aperture
- 13.5 Spatial Profiles
- 13.6 Line Spread Functions
- • 13.7 Spectral Purity, Order Confusion, and Peculiarities
- • 13.8 MAMA Spectroscopic Bright Object Limits
Chapter 14: Imaging Reference Material
- • 14.1 Introduction
- • 14.2 Using the Information in this Chapter
- 14.3 CCD
- 14.4 NUV-MAMA
- • 25MAMA - FUV-MAMA, Clear
- • 25MAMAD1 - FUV-MAMA Pseudo-Aperture
- • F25ND3 - FUV-MAMA
- • F25ND5 - FUV-MAMA
- • F25NDQ - FUV-MAMA
- • F25QTZ - FUV-MAMA, Longpass
- • F25QTZD1 - FUV-MAMA, Longpass Pseudo-Aperture
- • F25SRF2 - FUV-MAMA, Longpass
- • F25SRF2D1 - FUV-MAMA, Longpass Pseudo-Aperture
- • F25LYA - FUV-MAMA, Lyman-alpha
- • 14.6 Image Mode Geometric Distortion
- • 14.7 Spatial Dependence of the STIS PSF
- • 14.8 MAMA Imaging Bright Object Limits
- Chapter 15: Overview of Pipeline Calibration
- Chapter 16: Accuracies
Chapter 17: Calibration Status and Plans
- • 17.1 Introduction
- • 17.2 Ground Testing and Calibration
- • 17.3 Ground Testing and Calibration
- • 17.4 Cycle 7 Calibration
- • 17.5 Cycle 8 Calibration
- • 17.6 Cycle 9 Calibration
- • 17.7 Cycle 10 Calibration
- • 17.8 Cycle 11 Calibration
- • 17.9 Cycle 12 Calibration
- • 17.10 SM4 and SMOV4 Calibration
- • 17.11 Cycle 17 Calibration Plan
- • 17.12 Cycle 18 Calibration Plan
- • 17.13 Cycle 19 Calibration Plan
- • 17.14 Cycle 20 Calibration Plan
- • 17.15 Cycle 21 Calibration Plan
- • 17.16 Cycle 22 Calibration Plan
- • 17.17 Cycle 23 Calibration Plan
- • 17.18 Cycle 24 Calibration Plan
- • 17.19 Cycle 25 Calibration Plan
- • 17.20 Cycle 26 Calibration Plan
- Appendix A: Available-But-Unsupported Spectroscopic Capabilities
- • Glossary