STIS Design Charles Proffitt

STIS Presentation 2 Outline of Topics Introduction Basic Structure of STIS Detectors MSM optical elements & observing modes Slits and Apertures Target Acquistions Lamps and Wavecals

STIS Presentation 3 Introduction to STIS Space Telescope Imaging Spectrograph Highly versatile spectrograph 3 detectors (can use only one at a time)  FUV MAMA ~ Å, 1024 x 1024, ~0.025” pixels  NUV MAMA ~ Å, 1024 x 1024, ~0.025” pixels  CCD ~ ,000 Å, 1024 x 1024, ~ 0.05” pixels Long slit 1st order spectra High dispersion UV echelle spectra Resolution  up to ~ 100,000 Also slit-less and imaging modes

STIS Presentation 4 STIS Operational History Replaced GHRS in Axial Bay 1 on Feb 14, 1997 during SM2 STIS Side 1 failed on May 16, 2001  4.25 years and ~ 42,000 hours of operation  Probable short in tantalum capacitor - completely disabled side 1  Failure inaccessible without removing STIS STIS Side 2 failed on August 3, 2004  3.25 years and ~ 27,000 hours of operation  Failure in Interpoint converter that supplies power to move mechanisms  STIS other wise appears to be healthy, but no way to move the mechanisms or get light to the detector  STIS now turned-off (except for heaters) to avoid applying power to bad component  Repair planned for SM4; will replace LVPS2 board

STIS Presentation 5 STIS Optical Bench

STIS Presentation 6

7 STIS Mechanisms Corrector/Focus mechanism  Separately adjustable in tip, tilt, and focus  Last used during SMOV2 in 1997  Will adjust during SMOV4 only if necessary Echelle Blocker  Keeps scattered light from unused detector’s echelles Mode Isolation Mechanism  Blocks direct light from MSM to MAMA unless desired Calibration Insert Mechanism (CIM) Slit Wheel Mode Select Mechanism (MSM)

STIS Presentation 8 STIS Slit Wheel Slit wheel is in a image plane 77 standard slit wheel positions defined in aperture table 45 distinct clear slits and apertures 7 ND slits 13 imaging filters 12 alternate rotations for barred apers Only a subset available for GOs For STIS the APERTURE keyword value refers to a unique slit wheel pos Some physical slits have multiple slit wheel APERTURE positions defined (e.g., barred and regular long-slit pos) Alternate pointings of HST at the same slit wheel position are captured in PROPAPER keyword (e.g., E1 aperture positions vs. regular positions). Sometimes called pseudo-aperture positions Usage differs from other instruments. In STIS slits & filters are not “optical elements” as far as most ops data bases are concerned.

STIS Presentation 9 Mode Select Mechanism Tilted cylinders allow MSM to rotate and “wobble” to allow tip/tilt of elements Rotation of large wheels more precise than tip-tilt of small actuators Repeatability still not perfect 21 optical elements in MSM 16 gratings & 1 PRISM 4 imaging mirrors 10 elements have order sorter filters For the 4 echelle modes, the cross- disperser is the element in the MSM Each optical element is intended for use with only 1 optical path & 1 detector Exceptions for echelle cross dispersers, but exceptions not used on-orbit

STIS Detectors

STIS Presentation 11 MAMA Detectors MAMA = Multi-Anode Microchannel Array  Photocathode produces electron when hit by individual photon  Microchannel plate turns electron into charge cloud (4 x 10 5 e - )  1K x 1K anode array detects and centroids charge cloud  1024 x 1024 pixels ~ ” pixel size - 25”x25” FOV  Can be subsampled to 2048 x 2048 Advantages of MAMA detectors  Good FUV and NUV sensitivity  Photon counting  no read-noise  Time-tag mode possible  Less sensitive to cosmic rays (just one more dark current count at worst)  Low dark current  More resistant to radiation damage than CCDs  (but maybe not completely immune to rad. damage)  No charge transfers (no CTI losses or tails)  High spatial resolution

STIS Presentation 12 MAMA Detectors Dis-advantages of MAMA detectors  Subject to damage if over-illuminated  Cannot operate during SAA (high count rate)  Difficult to manufacture STIS MAMA peculiarities  STIS MAMAs have optical isolators that scintillate from cosmic rays  This forces STIS MAMA low voltage to be turned off during SAA  Prevents STIS MAMAs from observing in any SAA impacted orbit  HV only on for one ~ orbit block per day  STIS NUV MAMA has high dark current due to long phosphorescent window glow excited by charged particle impacts

STIS Presentation 13 FUV MAMA Detector

STIS Presentation 14 MAMA Anode Array Pulse location positions are centroided using anode grid Data routinely sub-sampled to 2048 x 2048 grid, but flat fielding issues prevent extra resolution from being useful Amount of charge, number of “folds”, and location used to choose “valid” events.

STIS Presentation 15 MAMA Detectors Micro channel plate consists of bundles of curved glass tubes 1. Photon hits photocathode, ejects electrons 2. Voltage across plate accelerates electrons down tubes 3. Electrons collide with walls, eject more electrons 4. Average gain of 4 x 10 5 (electrons out per photon event) 5. Size and location of charge cloud used to distinguish valid events.

STIS Presentation 16 Differences Between MAMAs FUV MAMA  CsI photocathode on Micro-channel Plate  Strongest response Å  Field electrode & repeller wire between window and photocathode NUV MAMA  CsTe 2 photocathode on inside of detector window  Slight defocus from lateral drift of electrons  No repeller wire or field electrode  Strongest response Å  Significant sensitivity down to 1150 Å  Intended as backup for FUV MAMA Unused backup modes to replicate FUV abilities much lower FUV throughput

STIS Presentation 17 MAMA Detectors MAMAs detect individual photons One event recorded per photon Invalid events are discarded ACCUM and TIME-TAG differ mostly in what gets saved  In ACCUM mode, each event increments memory location for that pixel. Only final accumulated image saved.  Pixel locations shifted on-orbit for orbital doppler correction  In TIME-TAG mode, position and time of each valid event are saved. Doppler correction done later. If HV is on, MAMA tubes continue to operate even when exposures are not in progress - events just aren’t recorded

STIS Presentation 18 MAMA Bright Object Limits MAMAs can be damaged by excessive illumination  Extracting too much charge too quickly, could limit future charge extraction, cause localized gain sag, decrease effective sensitivity  Very large count rates can produce gas in tube, perhaps leading to catastrophic short circuit or gas venting to aft-shroud  CARD (Constraints and Restrictions Document) Limits  Global > 1.5e6 counts for 1 second  Local > 500 counts/lo-res-pixel/s over 4x4 area for > 30 s  Detectors become non-linear at > 300,000 counts/s  Science calibration difficult  Lower screening limits set for operations  Global limit 200,000 counts/sec for most modes  30,000 counts/sec for 1st order point sources  Local limit 75 (spec) or 100 (imaging) counts/lo-res-pixel/s Brightest pixel  Lower global limits (80,000/12,000) for irregularly variable objects

STIS Presentation 19 Automatic BOP Mechanisms Bright Scene Detector (BSD)  Every 32nd anode wire monitored by special circuit  Unaffected by high count rates that may saturate normal counting electronics  Detector safed if this monitor is triggered  Trigger equivalent to uniform ~ 2x10 6 cnt/s global rate  Sparse coverage - bright source could fall between monitored rows  Spectrum at right location could safe detector with only ~ 120,000 counts/s Software Global Monitor (SGM)  Uses event counters giving global rate to detect overlight  Monitors all counts (valid or invalid) above set threshold voltage  Triggers at 1x10 6 c/s (equivalent to ~ 580,000 valid c/s)  Affected by non-linearity at high counts rates (> 4x10 6 c/s)  Can shut down detector within 0.1 s Local Rate Check Image (LRC)  300 ms image taken before each MAMA observation  Rebinned 2x2 and 4x4 and brightest pixels compared to limits  Failure of LRC causes detector to be shuttered & and any lamps to be turned off  Only shuttered image lost  Check only done at start of observation

STIS Presentation 20 STIS MAMA Detectors STIS MAMA Detector Performance Characteristics Characteristic FUV-MAMA Performanc e NUV-MAMA Performan ce Photocathode CsI Cs 2 Te Wavelength range Å Å Pixel format 1024 x x 1024 Pixel size25 x 25 µm 25 x 25 µm Image mode pixel plate scale~0.0245” x ” ~0.0245” x ” Field of view 25.1 x 25.3” 25.1 x 25.4” Quantum 1216 Å 2537 Å D ar k count 5 x to 1 x c/s/pixel8 x to 1.7 x c/s/pixel Global count-rate linearity limit 1 285,000 counts/s285,000 counts/s Local count-rate linearity limit 1 ~220 counts/s/pixel~340 counts/s/pixel Rate at which counting shows 10% deviation from linearity. These count rates are well above the bright-object limit.

STIS Presentation 21 STIS CCD STIS CCD: 1024 x 1024 thinned backside illuminated SITe CCD Thermal electric cooler (TEC) to allow CCD to operate at -83 C. Includes overscan region to ease bias removal CCD accumulates charge in each pixel and then is readout by transferring charge row by row to readout register and then pixel by pixel to amplifier

STIS Presentation 22 CCD Characteristics ACCUM mode only - image read out after exposure Can read out subarrays Cosmic ray hits can affect numerous pixels  Often need to CR-SPLIT images Some charge can lag during readout.  Charge Transfer Inefficiency (CTI)  Gets worse as CCD accumulates radiation damage on-orbit  Affects fluxes and causes tails in images Thinned CCD has good UV sensitivity, but too transparent in red - photons scatter in chip  Interference fringing in IR  Red light halo

STIS Presentation 23 STIS CCD STIS CCD Detector Performance Characteristics Characteristic CCD Performanc e Architecture Thinned, backside illuminated Wavelength range ~ ,000 Å Pixel format 1024 x 1024 illuminated pixels Field of view 52 x 52 arcseconds Pixel size 21x 21 µm Pixel plate scale arcseconds Quantum efficiency ~ Å ~ Å ~ 9000 Å Dark count at -83° C0.007 e-/s/pixel (but varies with detector T) Read noise (effective valu e s)5.4 e- rms at GAIN=1 (1 e- of which is pattern no i se) 7.6 e- rms at GAIN=4 (0.2 e- of which is pattern noise) Full well 144,000 e- over the inner portion of the detecto r 120,000 e- over the outer portion of the detector Saturation lim i t 33,000 e- at GAIN=1 (16 bit A-to-D limit) 144,000 e- at GAIN=

MSM Optical Elements and Observing Modes

STIS Presentation 25 STIS Observing Modes Echelle Modes  E140M, E140H  E230M, E230H 1st Order and PRISM Modes  G140L, G230L, G230LB, G430L, G750L  G140M, G230M, G230LM, G430M, G750M  NUV Prism Imaging Modes  Imaging mirror for each detector  2 for FUV - clear and filtered Acquistion modes  ACQ mode uses image to align target with standard slit  ACQ/Peak modes center target in small slit

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STIS Presentation 30 1st Order vs Echelle 1st order gratings (m=1)  Low blaze angle, fine ruling  Large free spectral range  Some use blocking filters to remove higher order Echelle gratings (orders m = )  High blaze angle, coarser ruling  Use higher order spectra for much higher dispersion  Smaller free spectral range per order~ /m  Use cross-disperser to separate orders  Can image many orders on detector at once  Flux calibration more difficult

STIS Presentation 31 Medium resolution 1st order gratings, need to be scanned in dispersion direction to cover full spectral range Echelle gratings, need to be scanned in cross-dispersion direction to cover all wavelengths For STIS L-modes, whole spectral range fits onto detector  G140L ~ Å  G230L ~ Å  G230LB ~ Å  G430L ~ Å  G750L ~ ,200 Å (larger contaminated by 2nd order light) Scanning of gratings

STIS Presentation 32 Dispersion, coverage, & throughput

STIS Presentation 33 Dispersion, coverage, & throughput

STIS Presentation 34 G140M & G230M Central Settings Only pre-defined grating tilts allowed  Prime settings will scan whole range (~10% overlap)  Secondary settings for special purposes

STIS Presentation 35 G230MB, G430M, G750M Cenwaves CCD M gratings, lower dispersion, but larger coverage than MAMA M gratings

STIS Presentation 36 Use of 1st order mode with long slit G750M observation of M84 (Radio Galaxy) nucleus  Bower et al. (1998), ApJL, 492, L111 Long slit (52X0.2) at 6581 CENWAVE across nucleus Shows N II and S II emission lines from disk Gives rotation curve with high resolution ~ 0.05”/pixel

STIS Presentation 37 Echelle mode CENWAVE settings Many secondary settings to allow flexibility.  Used frequently by GOs E140M covers ~ 1123 to 1710 Å with one setting

STIS Presentation 38

STIS Presentation 39 STIS Echelle Spectra E140M LINE lamp spectrum E140M Stellar Spectrum

Apertures and Filters

STIS Presentation 41 STIS Slit Wheel Very large number of apertures Slit name convention, e.g, 52X2  “length in spatial direction” x “length along dispersion direction”  F preceeds name of filtered apertures Full list of slit wheel position names 0.05X29 F25CIII 0.1X X0.06FPA 1X X X29 F25CN X X0.06FPB 1X0.2 52X0.05F1 0.2X29 F25CN X X0.06FPC 2X2 52X0.05F2 0.05X31NDA F25LYA 0.1X X0.06FPD 6X X X31NDB F25MGII 0.2X0.05ND 0.2X0.06FPE 6X0.2 52X0.1F1 F28X50LP F25ND3 0.2X X0.2FPA 6X0.5 52X0.1F2 F28X50OII F25ND5 0.2X X0.2FPB 6X6 52X0.2 F28X50OIII F25NDQ 0.2X X0.2FPC 31X0.05NDA 52X0.2F1 52X0.1B0.5 F25QTZ 0.2X X0.2FPD 31X0.05NDB 52X0.2F2 52X0.1B1.0 F25SRF2 0.3X0.05ND 0.2X0.2FPE 31X0.05NDC 52X0.5 52X0.1B X X0.05N45 52X0.5F1 0.3X X0.05P45 52X0.5F2 0.3X0.2 36X0.6N45 52X2 0.5X0.5 36X0.6P45 52X2F1 50CCD 52X2F2 50CORON  Some wheel position “APERTURES” have multiple target positions defined for same slit wheel setting. These are not included in this list.

STIS Presentation 42 Slits for 1st order spectroscopy First order observations usually use 52” long slits, 52X2, 52X0.5, 52X0.2, 52X0.1, 52X0.05  52X2 for best absolute photometry  Smaller slits for cleaner LSF or extended targets The 52” slits all have a pair of fiducial bars  Alternate slit rotations (rotate aperture wheel) are defined to bring either fiducial bar closer to center, and target behind bar

STIS Presentation 43 Barred aperture positions Append F1 or F2 to aperture name (e.g. 52x0.2F1) Rotation of aperture wheel gives different slit angle Only 52X0.2F1 “supported”, but other bars “available”

STIS Presentation 44 Alternate Aperture Positions For some apertures, multiple positions defined, but using same aperture wheel rotation  For STIS these are often referred to as pseudo-apertures. In image header in PROPAPER keyword  APERTURE keyword still set to name of physical aperture. E1 apertures for lower CTI D1 apertures for lower FUV dark current

STIS Presentation 45 STIS Aperture Selection, continued Echelle observations usually use short slits  0.2X0.2 for best throughput & photometry  Smaller slits matched to each grating for better LSF  0.2X0.06 for E140M & E230M; 0.2x0.09 for E140H & E230H  Smallest slit 0.1X0.03 to maximize resolution  Small ND slits 0.2X0.05ND (100X) and 0.3X0.05ND (1000X)  FP-SPLIT slits (0.2X0.2FPA-E & 0.2X0.06FPA-E) to dither target along dispersion direction - solve for fixed-pattern noise. Dispersion

STIS Presentation 46 STIS Aperture Selection - cont Most apertures can be used with most gratings  NUV-PRISM and 1st order gratings often used slitless  Can use long slits with echelle for spatially resolved observations of emission line sources Filters are also in aperture wheel and can be crossed with gratings, (e.g., use long-pass filter to block geo- coronal lyman-alpha in slitless G140L images)

STIS Presentation 47 Wide slits and extended sources With wide slit, cannot separate spatial offsets in dispersion direction from wavelength shifts Wide slit observations of extended objects degrade spectral resolution For emission line sources can take advantage of this to do emission line images. STIS G750M × 2 Spectral Image of SN1987A. This shows the images of the inner circumstellar ring in [OI], Hα, [NII], and [SII]. Diffuse Hα emission from the LMC fills the 52 × 2 slit, and broad Hα emission from the SN is also visible. The continua of stars produce the horizontal bands. The image shown is a 950 × 450 subsection of the 1024 × 1024 image. (Figure courtesy of Jason Pun and George Sonneborn, see also Sonneborn et al. 1998, ApJ, 492, L139).

STIS Presentation 48 MAMA Imaging FUV Imaging  FUV imaging capabilities similar to ACS SBC  Solar blind, but red-leak may be worse than specs NUV Imaging  Some sensitivity at FUV wavelengths  At long, overlaps with ACS/HRC and WFC3/UVIS abilities

STIS Presentation 49 STIS CCD Imaging Modes CCD Imaging  Primarily needed for target ACQs, but also for science  Between SM2 and SM3B (ACS install), the unfiltered STIS CCD was the most sensitive imaging instrument on HST  Only limited filters (OIII has significant red leak)  Also ND filters

STIS Presentation 50 Imaging Coronagraphy Coronagraphic Mask in filter wheel for use with CCD imaging  Unfiltered coronagraphy only, cannot cross with other filters. Predefined aperture locations, WEDGEA1.0, etc. Imaging mode mirror has Lyot stop, but secondary and spider not aphodized.