astronomical observational techniques and instrumentation
DESCRIPTION
Astronomical Observational Techniques and Instrumentation. RIT Course Number 1060-771 Professor Don Figer X-ray Astronomy. Aims of Lecture. review x-ray photon path describe x-ray detection describe specific x-ray telescopes give examples of x-ray objects. X-ray Photon Path. - PowerPoint PPT PresentationTRANSCRIPT
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Astronomical Observational Techniques and Instrumentation
RIT Course Number 1060-771 Professor Don Figer
X-ray Astronomy
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Aims of Lecture• review x-ray photon path• describe x-ray detection• describe specific x-ray telescopes• give examples of x-ray objects
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X-ray Photon Path
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Atmospheric Absorption• X Rays are absorbed by Earth’s atmosphere
– lucky for us!!!
• X-ray photon passing through atmosphere encounters as many atoms as in 5-meter (16 ft) thick wall of concrete!
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X RaysVisible Light
How Can X Rays Be “Imaged”?• X Rays are too energetic to be reflected “back”, as is possible
for lower-energy photons, e.g., visible light
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X Rays (and Gamma Rays “”) Can be “Absorbed”
• By dense material, e.g., lead (Pb)
Sensor
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Imaging System Based on Selective Transmission
Input Object(Radioactive Thyroid)
Lead Sheet with Pinhole “Noisy” Output Image(because of small number
of detected photons)
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How to “Add” More Photons1. Make Pinhole Larger
Input Object(Radioactive Thyroid
w/ “Hot” and “Cold” Spots)
“Fuzzy” Image Through Large Pinhole
(but less noise)
“Noisy” Output Image(because of small number
of detected photons)
“Fuzzy” Image
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How to “Add” More Photons2. Add More Pinholes
• BUT: Images “Overlap”
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How to “Add” More Photons2. Add More Pinholes
• Process to combine “overlapping” images
Before Postprocessing After Postprocessing
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Coded Aperture Mask• A coded aperture mask can be used to make images by relating intensity
distribution to the geometry of the system through post-processing, as described in the thyroid example.
• Six coded aperture mask instruments are operational in space: XTE-ASM, HETE-WXM, SWIFT-BAT and the three instruments on INTEGRAL.
• EXIST is being considered as a Black Hole Finder Probe in NASA's Beyond Einstein program.
Instrument1 Principle Investigator Science Operational Period
Detector/ E-range
(keV) E-resolution
Pattern3 Config4
Mask mat.
FOV5 (degrees)/ Ang. Res. (arcmin)
Det. Area (cm2)
No. of
Modules6
Instruments flying
ASM RXTE
H. Bradt (MIT) USA
XB,AGN,GRB 95- PSPC 2-10 25%@6 keV
ORA R|S|1 Al/Au
6X90 (HM) 3X15
90 3
WXM HETE
E. Fenimore (LANL) & N. Kawai (RIKEN) USA & Japan
GRB, X-ray bursts
00- PSPC 2-30 15%@6 keV
ORA(33%) R|S/C|1 Al/Au
90X90 (ZR) 40
400 2
IBIS INTEGRAL
P. Ubertini (IAS) Italy
XB,AGN 02- CdTe/CsI 20-10000 8% @ 100 keV
MURA R|C W
8X8 (FC) 12
2500 1
SPI INTEGRAL
V. Schoenfelder (MPE) Germany
Galactic diffuse emission
02- Ge 20-8000 0.2% @ 1.33 MeV
HURA H|C W
16 (FC) 120
500 1
JEM-X INTEGRAL
N. Lund (DSRI) Denmark
XB,AGN 02- PSPC 3-35 13%@10 keV
ORA(25%) H|C W
4.8 (FC) 3
500 2
BAT SWIFT
N. Gehrels (GSFC) USA
GRB, hard X-ray survey
04- CdZnTe 15-150 6 keV throughout
URA H|C
120 17
5200 1
Instruments being studied
EXIST Balloon
J. Grindlay (Harvard) USA
Survey CdZnTe 5-600 1% @ 100 keV
20X6 (HM) 5
2500 4
1Instruments between parentheses experienced difficulties in flight 2 XB - galactic X-ray binaries, GRB - gamma ray burst phenomenon, ASM - all-sky monitoring, SSM - selected-sky monitoring, AGN - active galactic nuclei, Technology - instrument technology, GC - the galactic center 3 Pattern: FZP = Fresnel Zone Plate, ORA = Optimized RAndom pattern, URA = Uniformly Redundant Array, HURA = Hexagonal URA; p = pseudo-noise subset, h = hadamard subset, tp = twin prime subset; triadic = near-URA with 0.33 open fraction 4 Configuration: R = rectangular, H = hexagonal, C = cyclic, S = simple, 1 = 1-dimensional 5 HM=full width at half maximum, ZR=full width at zero response, FC=full width of fully coded field of view 6 Number of modules
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Would Be Better to “Focus” X Rays• Could “Bring X Rays Together” from Different Points in
Aperture– Collect More “Light” Increase Signal– Increases “Signal-to-Noise” Ratio
• Produces Better Images
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X Rays and Grazing Incidence
X Ray at “Grazing Incidenceis “Deviated” by Angle
(which is SMALL!)
X-Ray “Mirror”
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Why Grazing Incidence?• X-Ray photons at “normal” or “near-normal” incidence
(photon path perpendicular to mirror, as already shown) would be transmitted (or possibly absorbed) rather than reflected.
• At near-parallel incidence, X Rays “skip” off mirror surface (like stones skipping across water surface)
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X-ray Collecting Mirrorsn.b., Distance from Front End to Sensor is LONG due to Grazing Incidence
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X-Ray Mirrors• Each grazing-incidence mirror shell has only a very small
collecting area exposed to sky– Looks like “Ring” Mirror (“annulus”) to X Rays!
• Add more shells to increase collecting area: create a nest of shells
“End” View of X-Ray Mirror
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X-Ray Mirrors• Add more shells to increase collecting area
– Chandra has 4 rings (instead of 6 as proposed)
• Collecting area of rings is MUCH smaller than for a Full-Aperture “Lens”!
Nest of “Rings” Full Aperture
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X-ray Detection
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The Perfect X-ray Detector• What would be the ideal detector for satellite-borne X-ray astronomy? It would
possess:– high spatial resolution – a large useful area, – excellent temporal resolution – ability to handle large count rates– good energy resolution – unit quantum efficiency – large bandwidth– output would be stable on timescales of years – internal background of spurious signals would be negligibly low– immunity to damage by the in-orbit radiation environment – no consumables– simple design– longevity– low cost– low mass – low power – no moving parts – low output data rate– (and a partridge in a pear tree)
• Such a detector does not exist!
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X-ray Detectors• Principle measurements
– flux– position– energy– time of arrival
• Specific types of detectors– gas proportional counter: x-ray photoionizes gas and induces voltage
spike in nearby wires– CCD: x-ray generates charge through absorption in silicon– microchannel plates: x-ray generates charge cascade through
photoelectric effect– active pixel sensor (i.e. CMOS hybrid detector array): x-ray generates
charge through absorption in silicon– single photon calorimeters: x-ray heats a resistive element an amount
equal to the energy of the x-ray
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X-ray Detector Materials• Light sensitive materials must be sensitive to x-ray energies
(~1-100 keV)– must allow some penetration– must have enough absorption or photoionization
• Good materials– gas– CZT (CdZnTe)– CdTe– silicon
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X-ray Image of Fe55 Source• For precise measurements of conversion gain (e-/ADU) or
Charge Transfer Efficiency (CTE), one often uses an Fe-55 X-ray source.
• Fe55 emits K-alpha photons with energy of 5.9KeV (80%) and K-beta photons with energy of 6.2KeV (20%). Impacting silicon, these will free 1616 and 1778 electrons, respectively.
Image of Fe55 x-rays obtained in the RIT Rochester Imaging Detector Lab (RIDL) with a silicon detector.
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Fe55 Experiment with Silicon Detector
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CCDs as X-Ray Detectors
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CCDs “Count” X-Ray photons• X-Ray events happen much less often
– fewer available X rays – smaller collecting area of telescope
• Each absorbed x-ray has much more energy– deposits more energy in CCD– generates many electrons
• Each x-ray can be counted– attributes of individual photons are measured independently
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Measured Attributes of Each X Ray1. Position of Absorption [x,y]2. Time when Absorption Occurred [t]3. Amount of Energy Absorbed [E]
• Four Pieces of Data per Absorption are Transmitted to Earth:
, , ,x y t E
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Why Transmit [x,y,t,E] Instead of Images?• Images have too much data!
– up to 2 CCD images per second– 16 bits of data per pixel (216=65,536 gray levels)– image Size is 1024 1024 pixels 16 10242 2 = 33.6 Mbps– too much to transmit to ground
• “Event Lists” of [x,y,t,E] are compiled by on-board software and transmitted– reduces required data transmission rate
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Image Creation• From event list of [x,y,t,E]
– Count photons in each pixel during observation• 30,000-Second Observation (1/3 day), 10,000 CCD frames are obtained
(one per 3 seconds)• hope each pixel contains ONLY 1 photon per image
• Pairs of data for each event are plotted as coordinates– Number of Events with Different [x,y] “Image”– Number of Events with Different E “Spectrum”– Number of Events with Different E for each [x,y] “Color Cube”
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X-ray Telescopes
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Chandra
Chandra in Earth orbit (artist’s conception)http://chandra.nasa.gov/
Originally AXAFAdvanced X-ray Astrophysics Facility
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Chandra Orbit• Deployed from Columbia, 23 July 1999• Elliptical orbit
– Apogee = 86,487 miles (139,188 km) – Perigee = 5,999 miles (9,655 km)
• High above LEO Can’t be Serviced• Period is 63 h, 28 m, 43 s
– Out of Earth’s Shadow for Long Periods– Longer Observations
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Chandra Mirrors Assembled and Aligned by Kodak in Rochester
“Rings”
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Mirrors Integrated into spacecraft at
TRW (NGST), Redondo Beach, CA
(Note scale of telescope compared to workers)
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Chandra ACIS CCD Sensor
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X-ray Objects
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First Image from Chandra: August, 1999Supernova remnant Cassiopeia A
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Example of X-Ray Spectrum
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Example of X-Ray Spectrum
Gamma-Ray“Burster”GRB991216
http://chandra.harvard.edu/photo/cycle1/0596/index.html
Counts
E
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Chandra/ACIS image and spectrum of Cas A
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Light Curve of “X-Ray Binary”
http://heasarc.gsfc.nasa.gov/docs/objects/binaries/gx301s2_lc.html