2.6 Scheduling Efficiency and Visit Orbit Limits
2.6.1: Reduced Gyro Mode
In 2024, HST was placed in reduced-gyro mode, which uses only one gyroscope in its attitude determination algorithm. While science observations are generally unaffected, the major impact is on schedulability due mostly to the reduced field-of-regard and a reduction in observational efficiency [link]. In summary, we expect the following considerations to affect proposers in Cycle 33 and beyond:
- It is expected that orbits longer than 5 contiguous orbits will be prohibitively difficult to schedule and so observers are recommended to split visits into small groups of orbits where possible.
- Similarly, strict orient and timing constraints may make visits impossible to schedule so observers are recommended to design their programs with as much flexibility as possible.
- Since target acquisition takes a few minutes longer compared to previous programs, users will have less available observing time per orbit in Cycle 33 going forward.
- Moving target and spatial scan rates are now limited to less than 5 arcsec per second.
- The Solar Avoidance Zone increases in size such that the telescope may now point no closer than ~60 degrees from the Sun, which may limit observations of certain Solar System objects (e.g., comets).
- See the HST RGM Primer for more information: The Hubble Space Telescope Primer for Cycle 33
2.6.2 Non-RGM Related Constraints
For the MAMA detectors, the 5 contiguous orbit limit is due to the number of South Atlantic Anomaly (SAA) free contiguous orbits. It is possible to have 6 of these orbits, however they are rare. Anything longer will never be schedulable. If a 6-orbit constraint is combined with any phase, timing and/or orient constraint restrictions then the visit will likely be unschedulable. STIS MAMA visits with 6 orbits require a compelling science justification and proposers must take into account the additional limitations that these longer visits place on observations and schedulability. See Section 2.6 for more information regarding MAMA scheduling constraints.
STIS CCD observations are possible to schedule in SAA impacted orbits. Therefore, there is slightly more flexibility with those observations being longer than 5 orbits with proper science justification. Scheduling longer orbit visits can be challenging, particularly when coupled with phase, time and/or orient constraints. Visits with 7 or more contiguous orbits can have very few scheduling opportunities per cycle (between zero and three), especially in RGM (see above).
2.6.3 Planning for Smaller Visits
Observers with programs using more than 5 orbits per target should take note of the following advice when splitting their observations into multiple visits:
- Target acquisition sequences will need to be repeated at the start of each visit when using small entrance apertures with STIS. Imaging and slitless spectroscopy do not normally require a target acquisition. Users should therefore account for additional overheads due to the increase in necessary target acquisitions.
- There exists the potential for some image rotation between visits unless the
SAME
ORIENT
AS
<first visits #> special requirement is used. WhenSAME
ORIENT
AS
is used, the accuracy is a few milliarcseconds. - Users are strongly encouraged to structure observations of 2-3 orbits duration each, unless longer visits are explicitly required to reach the stated science goals.
- Moving targets and spatial scanning: As of Cycle 28, limitations due to the gyro configuration of HST and its pointing control system restrict visits on moving targets to no more than two contiguous orbits. For similar reasons, for spatial scanning programs, each visibility period must have at least 6 minutes of time under FGS control (i.e., 6 minutes without scanning).
In structuring their programs, observers should carefully consider the positional accuracies that will be required. Acquisitions of point-source targets are generally accurate to ~10 milliarcseconds (see Section 8.2), and somewhat greater accuracy can be achieved by using a peakup in a small aperture (Section 8.3; see also the summary in Table 16.5). Within a given visit, HST pointing is generally very stable (~5 milliarcseconds rms), and small angle maneuvers can be similarly accurate (Section 8.2.3). For most single, non-variable point-source targets, a long series of exposures could, in principle, be obtained either in a single long (but difficult to schedule) visit or in two or more shorter visits, with somewhat shorter total exposure time but greater schedulability. If there are several different, closely-spaced targets to be observed (requiring slight movements of the telescope but using the same guide stars), and if very precise offsets (few milliarcsecond accuracy) between the different targets are required, then it might be desirable to observe all the targets in a single long visit. If such precise offsets are not required; however, then the observations could be obtained in separate shorter visits (e.g., with one target per visit). In cases where a target acquisition is performed for slit spectroscopy, one should follow the same procedure for the target acquisition in the subsequent visits as in the first.
Visits can be scheduled close in time by specifying the GROUP
WITHIN
visit requirement. Timing constraints of this type, however, should be used only if required by the science, since overconstraining visits affects the ability to schedule efficiently. All timing, orientation, and scheduling requirements must be identified and justified in the Phase I proposal.
-
STIS Instrument Handbook
- • Acknowledgments
- Chapter 1: Introduction
-
Chapter 2: Special Considerations for Cycle 33
- • 2.1 Impacts of Reduced Gyro Mode on Planning Observations
- • 2.2 STIS Performance Changes Pre- and Post-SM4
- • 2.3 New Capabilities for Cycle 33
- • 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
- • 8.1 Introduction
- • 8.2 STIS Onboard CCD Target Acquisitions - ACQ
- • 8.3 Onboard Target Acquisition Peakups - ACQ PEAK
- • 8.4 Determining Coordinates in the International Celestial Reference System (ICRS) Reference Frame
- • 8.5 Acquisition Examples
- • 8.6 STIS Post-Observation Target Acquisition Analysis
- 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
-
13.3 Gratings
- • 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
-
13.4 Apertures
- • 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
-
14.5 FUV-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 STIS Installation and Verification (SMOV2)
- • 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
- • 17.21 Cycle 27 Calibration Plan
- • 17.22 Cycle 28 Calibration Plan
- • 17.23 Cycle 29 Calibration Plan
- • 17.24 Cycle 30 Calibration Plan
- • 17.25 Cycle 31 Calibration Plan
- • 17.26 Cycle 32 Calibration Plan
- Appendix A: Available-But-Unsupported Spectroscopic Capabilities
- • Glossary