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ISAS to be launched on Feb. 8th, 200 Hakucho (1979) Tenma (1983) Ginga (1987) ASCA (1993) titute of Space and Astronautical Science

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ISAS. Astro-E. Hakucho (1979). Tenma (1983). to be launched on Feb. 8th, 2000. Ginga (1987). ASCA (1993). Institute of Space and Astronautical Science. 5.4 m. 6.5 m. Total Weight 1670 kg. - PowerPoint PPT Presentation

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Page 1: ISAS

ISAS

to be launched on Feb. 8th, 2000

Hakucho (1979)

Tenma (1983)

Ginga (1987)

ASCA (1993)

Institute of Space and Astronautical Science

Page 2: ISAS

The Astro-E mission is the fifth in a series of Japanese X-ray astronomy missions, following the Hakucho, Tenma, Ginga and ASCA satellites. It is scheduled to be launched on Feb. 8th 2000 by the M-V launch vehicle from Kagoshima Space Center (KSC), Japan.

Astro-E features excellent sensitivity, with high throughput over an unprecedented wide energy band from 0.5 keV to 600 keV. This wide bandpass, combined with high resolution spectroscopic capabilities, makes Astro-E a unique tool capable of addressing a wide variety of fundamental subjects in astrophysics, involving the origins of elements and structures in the Universe as well as the evolution and dynamics of these structures.

Astro-E

5.4 m

6.5 m

Total Weight 1670 kg

Page 3: ISAS

Development of Astro-E

International Collaborations•X-ray Telescope (XRT) [Nagoya Univ., NASA/GSFC, ISAS]

•X-ray Micro-calorimeter (XRS) [ISAS, NASA/GSFC, Univ. of Wisconsin,

Tokyo Metropolitan Univ., Riken]

•X-ray CCD (XIS) [Kyoto Univ., Osaka Univ., ISAS, MIT]

•Hard X-ray Detector (HXD) [Univ. of Tokyo, ISAS, RCNP]

•Operation and Data processing [ISAS, NASA/GSFC]

Astro-E was developed at Japan’s Institute of Space and Astronautical Science (ISAS) in an extensive collaboration between scientists from Japan and the United States.

Page 4: ISAS

Astro-E’s InstrumentsAstro-E carries five X-Ray Telescopes (XRTs). These telescope modules provide the soft X-ray images on the focal-plane instruments. One telescope module (XRT-S) feeds the X-ray Spectrometer (XRS); the other modules (XRT-I) have X-ray Imaging Spectrometer (XIS) units at their focal planes. At the same time, the Hard X-ray Detector (HXD) measures high-energy (hard) X-rays.

XRT-I

XRT-S

XRS

HXD

XIS

Page 5: ISAS

6.5m

Extendible Optical Bench (EOB)

The focal length of the telescope is

4.75 m for the XIS and 4.5 m for the

XRS. These telescopes are mounted

on an extendible optical bench.

Because of the limited length available

within the rocket nose fairing, the

optical bench is “telescoped” inside

the space craft during the launch and

will be extended by 1.5 m in orbit to

achieve the proper focal lengths.

Page 6: ISAS

Astro-E Satellite

(photo by ISAS)

Page 7: ISAS

(photo by ISAS)

Page 8: ISAS

Astro-E’s Orbit Astro-E will be, first, put into a transfer orbit of ~250 km perigee and ~550 km apogee. After three V operations at apogee, the final orbit will be approximately circular with ~550 km altitude and ~31 degree inclination.

• 180 deg attitude maneuver• Spin up• Satellite Separation

perigee up

Page 9: ISAS
Page 10: ISAS

X-ray Space Observatories in the New Millennium

Energy Resolution AreaImagingQuality

Energy Range

HighBroadHighLargeAstro-EChandraXMM

Page 11: ISAS

Effective Area of High Resolution Instruments

Page 12: ISAS

XRT-S + XRS XRT-I + XIS HXD

Energy range 0.4-12 keV 0.5 - 12 keV 10-600 keV

Effective area 190 cm2 1300 cm2 160cm2 (<30 keV) 330cm2 (>40 keV)

Focal Length 4.5 m 4.7 m

HPD of PSF 2' 2'

Energy resolution 12 eV at 6 keV 120 eV@ 6 keV 3.5 keV @ 10 keV ~9% @ 662 keV

Field of view 1.9' x 4.2' 19' x 19' 0.56 x 0.56 Åã @< 100 keV

4.6 x 4.6Åã @>200 keV

Pixel size 0.94' x 0.24' 1.1" x 1.1"

Number of pixels 2 x 16 1024 x 1024

Time resolution 30É sec 8 ms - 8 sec 30.5 - 61É sec

Astro-E Instruments

Page 13: ISAS

X-ray Telescopes (XRT)

(Photo by ISAS)

Astro-E X-ray telescopes consist of nested conical thin-foil mirrors based on a similar design concept to the ASCA telescopes, but with several improvements. The half power-diameter (HPD) is better than ASCA's by about a factor of two. The ratio of the focal length to the diameter is smaller, making the grazing angles smaller. This leads to better reflectivity for higher photon energies. The focal lengths of 4.5 m for the XRS and 4.75 m for the XIS give effective areas of ~500 cm2 at 1.5 keV and ~300 cm2 at 8 keV for a single telescope.

[Nagoya Univ., NASA/GSFC, ISAS]

Page 14: ISAS

ASCA(4)

Astro-E(4XIS)

Astro-E XRTArea: 2 x ASCA at 7keVHPD 2 arcmin (ASCA 3.6 arcmin)

The effective area of XRTs

The effective area of XRTs for Astro-E, ASCA, XMM and Chandra .

XMM

Chandra

Astro-E(XRS)

Page 15: ISAS

XRT Final Configuration on the satellite

XRT-S

XRT-I (photo by ISAS)

Page 16: ISAS

X-ray Spectrometer (XRS)

The XRS is a cryogenic X-ray detector system utilizing a microcalorimeter array of 32 pixels operating at 60 mK. An energy resolution of about 12 eV at 6 keV is obtained across the array.

The micro calorimeter array employed in the XRS is the first such instrument to fly in a satellite. Over broad range of energies, ~0.4 to 12 keV, it has an unprecedented energy resolution of 8-14 eV. XRS allows us to study chemical composition and dynamics of cosmic hot plasmas to the highest level, never achieved in the past.

5.34 mm(4.1’)

2.48 mm (1.9’)

[ISAS, NASA/GSFC, Wisconsin Univ., Tokyo Metro Univ., Riken] (Photo by NASA/GSFC)

Page 17: ISAS

The microcalorimeter in the XRS detects the temperature increase due to absorption of a single X-ray photon. The small heat capacities and low temperature lead to very small fluctuations, resulting in higher energy resolution compared to ordinary semiconductor devices. The XRS can resolve very small energy differences of X-ray photons.

Heat Sink, TSX-ray PhotonThermal Conductance, GX-ray AbsorterHeat Capacitance, CThermometer

Silicon Pixel

Silicon Support Beams

X-Ray Absorber(HgTe)

Implanted Traces

Implanted Thermistor

Silicon Spacer

Principles of the XRS

Page 18: ISAS

 

  The microcalorimeter must be operated at about 60 mK. A unique three-stage cryogenic system consisting of solid neon, liquid helium, and an adiabatic de-magnetization refrigerator is adopted to provide cooling for the detector. The design of the neon tank is optimized to work about 2 years in orbit, which determines the lifetime of the whole cryogenic system.

(photo by ISAS)

Page 19: ISAS

XRS Array Assembly

XRS Flight Array Installed in CTS

Number of pixels : 32Absorber: HgTe (8 µm)Pixel dimensions: 1.23 0.32 mm

(57” 15”)Filling factor: 94.6 %

(Photo by NASA/GSFC)

Page 20: ISAS

Energy resolution of the XRS

E = 8-9 eV below 3keVE = 11-14 eV at 8keV

Energy (keV)

0 10 155

Page 21: ISAS

Astro-E/XRSSimulation ofCentaurus Cluster100 ksec exposure CCD

Response

He-like FeKZ = 0.01(3000 km/sec)

Expected performance of the XRS

Page 22: ISAS

X-ray Imaging Spectrometer (XIS)

The XIS plays key role in simultaneous imaging and spectroscopic observations over the energy range of 0.5 - 12 keV. Many efforts have been made to improve the performance of ASCA’s X-ray CCDs and their related electronics. Astro-E’s CCD is front-illuminated frame-transfer device with 1024x 1024 pixels. Each pixel is 24 µm square and the size of the CCD is 25 mm x 25 mm. Energy resolution is ~120 eV at ~ 8 keV.

[Kyoto Univ., Osaka Univ., ISAS, MIT]

(photo by ISAS)

Page 23: ISAS

XIS CCD Assembly

(photo by MIT)

Page 24: ISAS

Hard X-ray Detector (HXD)

HXD is a collimated instrument sensitive in the band of 10 keV to 600 keV. It is designed to minimize the detector backgrounds by its improved shielding. The HXD sensor is consisting of 16 main detectors and the surrounding 20 crystal scintillators for active shielding. Each detector unit consists of two types of detectors: Gadolinium silicate (GSO) crystal buried deep in the bottom of the Well-shape Bismuth germanate (BGO) crystal, and PIN silicon diodes located inside the well.

[Univ. of Tokyo, ISAS, RCNP]

(photo by ISAS)

Page 25: ISAS

The silicon PIN diode on GSO. covers lower energy band below ~40 keV, while the GSO is sensitive above ~30 keV.

The HXD is a phoswich counter with the “well-type” structure. The BGO crystal actively shields the detection part. It also acts as an active collimator, which provides a fine field of view with a small amount of passive material.