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Science team George Rieke (U of A, Lead) Gillian Wright (ROE, Instrument PI and Co-lead) Tom Greene (NASA-Ames) Margaret Meixner (STScI) Mike Ressler (NASA-JPL, Instrument Scientist) Torsten Boeker (ESA-ESTEC) Thomas Henning (MPIA) Luis Colina (CSIC-IEM) STScI Instrument team
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Science team George Rieke (U of A, Lead) Gillian Wright (ROE, Instrument PI and Co-lead) Tom Greene (NASA-Ames) Margaret Meixner (STScI) Mike Ressler (NASA-JPL, Instrument Scientist) Torsten Boeker (ESA-ESTEC) Thomas Henning (MPIA) Luis Colina (CSIC-IEM) STScI Instrument team Christine Chen (APT/ETC) Scott Friedman (Commissioning) Karl Gordon (Calibration) Dean Hines (Operations) Rachel Anderson Misty Cracraft MIRI is a NASA/JPL-led partnership with a European Consortium sponsored by ESA NASA provides focal planes, signal chain Consortium provides optical bench assembly MIRI Observing Templates C. H. Chen
MIRI Operating Configurations • Imaging • = 5 - 27 m wavelength range • Diffraction limited imaging with 0.11” pixels • ~2 square arcmin field of view • Coronagraphy • Three 4 Quadrant Phase Masks (10.65, 11.4, and 15.5 m) • One Lyot Coronagraph (23 m) • Low Resolution Spectroscopy (LRS) • R ~ 100 from = 5 - 10 m • Medium Resolution Spectroscopy (MRS) • = 5 - 27 m wavelength range, goal to reach = 28.3 m • Integral field spectroscopy with fields of view of 3” or more • R ~ 3000 - 1000 from = 5 - 27 m C. H. Chen
MIRI FOV on the Sky • For more information, see “Mid-infrared Instrument (MIRI) Operations Concept Document” Rev C edited by C. H. Chen JWST-STScI-00910 C. H. Chen
MIRI Data Format Nominal Data File Coordinates In Final Format Nominal Data File Coordinates (w/Ref Output) • Reference Pixels - four pixels at the beginning and end of each row with no light sensitivity, one for each data output • Reference Output pixels - “blind” pixels interleaved with light-sensitive pixels that use a separate data output C. H. Chen
MIRI Readout Patterns • FASTMode • Each pixel in the (sub-)array is sampled once and that value is returned • Full frame time 2.775 sec • Will be used to observe bright targets • SLOWMode • Each pixel in the (sub-)array is sampled 10 times, the middle 8 samples are averaged together and returned • Full frame time 27.75 sec • Will be used to observe faint targets C. H. Chen
Imaging Astronomical Observation Requests • Target acquisition • Current implementation does not include target acquisition for direct imaging • The smallest subarrays (SUB64 and SUB128) may require target acquisition • User will specify TA source coordinates, TA filter, and expected brightness for the TA source in TA filter • Filter • User will select based on the science justification • Subarray • User will select based on the science justification and the brightness of the target, with guidance from ETC/APT software • Readout Pattern • User will select based on the science justification and the brightness of the target with guidence from ETC/APT software • Dither Pattern • User will select based on science justification C. H. Chen
Imaging: Filter Selection C. H. Chen
Imaging: Subarray Selection • For more information, see “MIRI Subarrays for Planetary Transits and Other Bright Objects” Rev. A by C. H. Chen, G. H. Rieke, & K. D. Gordon, JWST-STScI-001757 C. H. Chen
Imaging: Dither Pattern Selection • Available Patterns • No Dither (for transiting extra-solar planets) • 5-Point Gaussian (SUB64, SUB128) • 12-Point Reauleaux (SUB256, BRIGHTSKY, or FULL array) • 311-Point Cycling Pattern (SUB256, BRIGHTSKY, or FULL array) • User specifies starting position in list of offsets and number of dither positions required • Available Pattern Sizes: S, M, L • Optimal pattern sizes exist based on the • For more information, see “MIRI Imaging Dither Patterns” Rev A by C. H Chen JWST-STScI-001657 C. H. Chen
Coronagraphic Astronomical Observation Requests • Target acquisition • User will specify TA source coordinates, TA filter, and expected brightness for the TA source in TA filter • For more information, see “Mid-Infrared Instrument (MIRI) Target Acquisition Strategies and Use Cases” by Gordon & Meixner, 2008, JWST-001407 • Coronagraph/Filter • User will select based on the science justification • Subarray • Will be automatically selected based on Coronagraph/Filter selection • Readout Pattern • User will select based on the science justification and the brightness of the target with guidance from ETC/APT software • Dither Pattern • No dither pattern is allowed C. H. Chen
Coronagraph: Coronagraph/Filter Selection 4QPM Lyot • User must select which of the following coronagraphs they would like to use: 4QPM at 10.65, 11.4, or 15.5 m or Lyot Coronagraph at 23 m C. H. Chen
LRS Astronomical Observation Requests • Target acquisition • User will specify TA source coordinates, TA filter, and expected brightness for the TA source in TA filter • For more information, see “Mid-Infrared Instrument (MIRI) Low Resolution Target Acquisition for Faint Sources” by Gordon, 2008, JWST-STScI-001347 • Filter • Is automatically set to “LRS Prism” • Subarray • User will select (either LRS-Slit or LRS-Slitless) based on the science justification and the brightness of the target, with guidance from ETC/APT software • Readout Pattern • User will select based on the science justification and the brightness of the target given guidance from ETC/APT software • Dither Pattern • If LRS-Slit, then user will select based on science justification C. H. Chen
LRS Slit vs LRS Slitless Observations Slitless Slit Target placed in the slit Target placed in the Lyot FOV • LRS Slit • LRS Slit Target Acquisition • FULL frame is readout • LRS Slitless • LRS Slitless Target Acquisition TBD • SLITLESSPRISM subarray is readout C. H. Chen
LRS Slit Observations: Dither Pattern Selection • Point Source/Staring • Always two positions in the slit • Always 1/3 and 2/3 of the way along the slit • Extended Source/Mapping • Customizable grid of positions • User gives number of positions parallel and perpendicular to the slit • User gives offset between slit positions in direction parallel and perpendicular to the slit • For more information, see “The LRS Dither Pattern ” by C. H. Chen JWST-STScI-001634 C. H. Chen
MRS Astronomical Observation Requests • Target acquisition • User will specify TA source coordinates, TA filter, and expected brightness for the TA source in TA filter • For more information, see “Mid-Infrared Instrument (MIRI) Target Acquisition Strategies and Use Cases” by Gordon & Meixner, 2008, JWST-001407 • Grating • User will select based on the science justification • Subarray • Only FULL array observations are allowed • Readout Pattern • User will select based on the science justification and the brightness of the target with guidance from ETC/APT software • Dither Pattern • User will select based on science justification C. H. Chen
10 arcseconds Each channel’s field of view is sliced, dispersed and detected. Channel 1 (4.9 - 7.7 mm) Channel 2 (7.4 - 11.8 mm) Channel 3 (11.4 - 18.2 mm) Channel 4 (17.5 - 28.8 mm) Wavelength/Velocity MRS Overview C. H. Chen
MRS: Grating Selection • Select one sub-band at a time (A-”short”,B-”medium”, or C-”long”) or ALL C. H. Chen
MRS: Dither Pattern Selection (TBD) Pattern 2 Pattern 1 • Pattern 1 - improved spatial sampling for all channels simultaneously • Pattern 2 - improved spatial and spectra sampling for one channel at a time (Ch 1, 2, 3, and 4 optimized patterns) • For more information, see “MIRI MRS Dither Patterns” by C. H. Chen & A. Glasse JWST-STScI-001871 C. H. Chen