STIS Design

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 ~ 1150 - 1700 Å, 1024 x 1024, ~0.025” pixels NUV MAMA ~ 1600 - 3200 Å , 1024 x 1024, ~0.025” pixels CCD ~ 1650 - 11,000 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

STIS Presentation 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 105 e-) 1K x 1K anode array detects and centroids charge cloud 1024 x 1024 pixels ~ 0.0245” 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


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 ~ 5 - 6 orbit block per day

STIS NUV MAMA has high dark current due to long phosphorescent window glow excited by charged particle impacts


FUV MAMA Detector


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.


MAMA Detectors

Micro channel plate consists of bundles of curved glass tubes1. 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 105 (electrons out per photon event)

5. Size and location of charge cloud used to distinguish valid events.


Differences Between MAMAs

FUV MAMA CsI photocathode on Micro-channel Plate Strongest response 1150-2000 Å Field electrode & repeller wire between window and photocathode

NUV MAMA CsTe2 photocathode on inside of detector window

Slight defocus from lateral drift of electrons No repeller wire or field electrode

Strongest response 1700-3200 Å Significant sensitivity down to 1150 Å Intended as backup for FUV MAMA

• Unused backup modes to replicate FUV abilities

• much lower FUV throughput


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


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


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 ~ 2x106 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 1x106 c/s (equivalent to ~ 580,000 valid c/s) Affected by non-linearity at high counts rates (> 4x106 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 MAMA Detectors

STIS MAMA Detector Performance Characteristics

Characteristic FUV-MAMA Performance NUV-MAMA Performance-----------------------------------------------------------------------------------------------------------Photocathode CsI Cs2TeWavelength range 1150-1700 Å 1600-3100 ÅPixel format 1024 x 1024 1024 x 1024Pixel size 25 x 25 µm 25 x 25 µmImage mode pixel plate scale ~0.0245” x 0.0247” ~0.0245” x 0.0248”Field of view 25.1 x 25.3” 25.1 x 25.4”Quantum efficiency25% @ 1216 Å 10% @ 2537 ÅDark count 5 x 10-6 to 1 x 10-4 c/s/pixel 8 x 10-4 to 1.7 x 10-3 c/s/pixelGlobal count-rate linearity limit1 285,000 counts/s 285,000 counts/sLocal count-rate linearity limit1 ~220 counts/s/pixel ~340 counts/s/pixel-----------------------------------------------------------------------------------------------------------1Rate at which counting shows 10% deviation from linearity. These count rates are well above the bright-object limit.


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


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 CCD

STIS CCD Detector Performance Characteristics

Characteristic CCD Performance------------------------------------------------------------------------------------------------Architecture Thinned, backside illuminatedWavelength range ~1600-11,000 ÅPixel format 1024 x 1024 illuminated pixelsField of view 52 x 52 arcsecondsPixel size 21x 21 µmPixel plate scale 0.05071 arcsecondsQuantum efficiency ~ 20% @3000 Å

~ 67% @6000 Å~ 29% @ 9000 Å

Dark count at -83° C 0.007 e-/s/pixel (but varies with detector T)Read noise (effective values) 5.4 e- rms at GAIN=1 (1 e- of which is pattern noise)

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 detector

120,000 e- over the outer portion of the detectorSaturation limit 33,000 e- at GAIN=1 (16 bit A-to-D limit)

144,000 e- at GAIN=4------------------------------------------------------------------------------------------------

MSM Optical Elementsand Observing Modes


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


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 = 66 - 747) 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


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 ~ 1150 - 1736 Å G230L ~ 1570 - 3180 Å G230LB ~ 1680 - 3065 Å G430L ~ 2900 - 5700 Å G750L ~ 5240 - 10,200 Å (larger contaminated by 2nd order light)

Scanning of gratings


Dispersion, coverage, & throughput


G140M & G230M Central Settings

Only pre-defined grating tilts allowed Prime settings will scan whole range (~10% overlap) Secondary settings for special purposes


G230MB, G430M, G750M Cenwaves

CCD M gratings, lower dispersion, but larger coverage than MAMA M gratings


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


Echelle mode CENWAVE settings

Many secondary settings to allow flexibility. Used frequently by GOs

E140M covers ~ 1123 to 1710 Å with one setting


STIS Echelle Spectra

E140M LINE lamp spectrum

E140M Stellar Spectrum

Apertures and Filters


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 names0.05X29 F25CIII 0.1X0.03 0.2X0.06FPA 1X0.06 52X0.050.09X29 F25CN182 0.1X0.06 0.2X0.06FPB 1X0.2 52X0.05F10.2X29 F25CN270 0.1X0.09 0.2X0.06FPC 2X2 52X0.05F20.05X31NDA F25LYA 0.1X0.2 0.2X0.06FPD 6X0.06 52X0.10.05X31NDB F25MGII 0.2X0.05ND 0.2X0.06FPE 6X0.2 52X0.1F1F28X50LP F25ND3 0.2X0.06 0.2X0.2FPA 6X0.5 52X0.1F2F28X50OII F25ND5 0.2X0.09 0.2X0.2FPB 6X6 52X0.2F28X50OIII F25NDQ 0.2X0.2 0.2X0.2FPC 31X0.05NDA 52X0.2F152X0.1B0.5 F25QTZ 0.2X0.5 0.2X0.2FPD 31X0.05NDB 52X0.2F252X0.1B1.0 F25SRF2 0.3X0.05ND 0.2X0.2FPE 31X0.05NDC 52X0.552X0.1B3.0 0.3X0.06 36X0.05N45 52X0.5F1 0.3X0.09 36X0.05P45 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.


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


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”


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 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.D

ispersion


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)


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 6581 52 × 2 Spectral Image of SN1987A. This showsthe images of the inner circumstellar ring in [OI], Hα, [NII], and [SII]. Diffuse Hαemission 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).


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 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


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.

STIS Design

Documents

Transcript of STIS Design