Upload
others
View
2
Download
0
Embed Size (px)
Citation preview
T.Takahashi, Astronomy with Radioactivies IV,2003
Soft Gamma-ray Detector (SGD)for the NeXT mission
Tadayuki Takahashi
Institute of Space and Astronautical Science
(ISAS, Japan)
g-rayDetector
1979 1983 1987 1993
2005
ISAS/U-Tokyo/SLAC/Hiroshima U./Osaka U./Saitama U./Riken/Kanazawa U. (the SGD collaboration)
2010?
and beyond…Astro-E2
T.Takahashi, Astronomy with Radioactivies IV,2003
Introduction- filling the sensitivity gap -
Gap-1 Gap-2
• Development of highly-sensitivedetector in Soft Gamma-ray energybands (sub-MeV & MeV) is crucialissue.
• Our Approach• Extend the energy coverage
from X-ray to higher energy(from Gap-1 to Gap-2)
• Multi-band observation (fromX-rays) is important (andproductive), to study theNON-THERMAL universe.
• Apply the developed-technology to higher energyband for the Gap-2
The NeXT (New X-ray Telescope) mission– Next generation “Multi-band” mission to studythe non-thermal universe
(6th X-ray satellite in Japan, hope to be launched in 2010)
T.Takahashi, Astronomy with Radioactivies IV,2003
Spectrometer
Hard X-ray Imager
SGD
What’s ‘next’ in the NeXT mission• Super Mirror + Hard X-ray Imager
• High resolution X-ray detector (FWHM = 3 eV at 6 keV)• Soft Gamma-ray Detector (30 keV - 600 keV) (+polarization)
Super Mirror ( 0.5-80 keV )
Hard X-ray Imager
focal length8 - 12 m
g-rayDetector
ISAS
30’’ HPD
T.Takahashi, Astronomy with Radioactivies IV,2003
137Cs
FWHM2.1 keV
662keV
High Resolution CdTe detector- New Detector Material for the future mission -
• High Z semiconductor (ZCd = 48, ZTe = 52)
-> Significant Progress in 1990’s(Takahashi et al. IEEE NS49, 3,2002, review by Takahashi &Watanabe, IEEE NS48, 4, 950, 2001)
see posters by Tanaka et al.and by Mitani et al.
ISAS projectHigh Energy Resolution
12.8mm
Fine Position Resolution
CdTe Gamma-ray Imager(pixel size 200 µm)
ISAS & Bonn U.
T.Takahashi, Astronomy with Radioactivies IV,2003
To improve the sensitivity in the sub-MeV region
Key issues:
HXD Concept (High Signal to Background ratio)• tight active shields (Well-type shield)• the collimated narrow field of view (0.5 degree at 100 keV, 4 degree at 500keV by a fine collimator and BGO)• Compton suppression for high energygamma-ray• the compound-eye configuration.
• Cosmic X-ray Background (CXB) from the FOV• Non X-ray Background (Internal Background)• Confusion Limit in the FOV/Error circle
How can we improve this for the NeXT?Internal Background limits the sensitivity.
Si
GSO
10-600 keV HXD for Astro E-2BGO
T.Takahashi, Astronomy with Radioactivies IV,2003
Semiconductor Compton Telescopefor the pointing observation…
Stack of Si strips
High Resolution CdTe pixels
If we replace GSO+Si PIN diode usedin the HXD by ….
CG by Yuriko S
Well-type Active shield
and put them into the well…
T.Takahashi, Astronomy with Radioactivies IV,2003
New Concept: Narrow FOV Compton Camera• Gamma-rays from the source comefrom the “narrow” FOV (0.5-3 degFWHM) (Direction is Given!)
Select two hits events andaccept only if
†
E2 =(E1+ E2)
1+(E1+ E2)(1- cosq)
mec2
No need to worry about the sequenceif scattering angle is below…
First scattering (E1) has lower energy
This condition is expected to get rid of most of internal background.
(Takahashi et al. 2003, SPIE, vol. 4851)(Adoption of Fine Coll. is still an option)
T.Takahashi, Astronomy with Radioactivies IV,2003
• Lower accidental coincidences• Imaging capability withan angular resolution of ~degree,→ Important for modeling the backgroundspectrum for the Non-Compton mode
Narrow FOV Compton Camera
T.Takahashi, Astronomy with Radioactivies IV,2003
• Lower accidental coincidences• Imaging capability withan angular resolution of ~degree,→ Important for modeling the backgroundspectrum for the Non-Compton mode
Narrow FOV Compton Camera •24 layers of 0.5 mm-thick Strip Strip detectors
•6 mm-thick CdTe Pixel (res. 1mm)
Effective Areatotal
one Compton+ Abs.
Polarization (Scattered at Si and absorped in CdTe)
(200 keV)
T.Takahashi, Astronomy with Radioactivies IV,2003
Key technologiesunder development
1. High resolution Silicon Strip detector2. High resolution CdTe pixels/strips
(see posters by Mitani and Tanaka)3. Low Noise ASIC 4. Signal extraction (bump bonding)
Si strip with a new ASIC
0
200
400
600
800
1000
12002x10
241Am
59.5 keV
Energy [keV]
13.9 keV
17.6 keV
21.0 keV
26.3 keV
0 10 20 30 40 50 60 70
ΔE =1.5keV(FWHM)
25mm/400micron pitch
Uno etal., 2003
Tajima et al. 2003, SPIE, 4851
Takahashi etal., IEEE, NS. 48, 3,2001
T.Takahashi, Astronomy with Radioactivies IV,2003
Compton Reconstruction
Tajima, Uno, Mitani, Nakazawa, Takahashi, Fukazawa et al.
T.Takahashi, Astronomy with Radioactivies IV,2003
Sensitivity of the NeXT mission0.3 - 600 keV
– High Sensitivity for both Line and Continuum
– Polarization measurement 100 ks
CasA
Line Cont.
This is not the end of the story…
68keV
T.Takahashi, Astronomy with Radioactivies IV,2003
Semiconductor Multi Compton Telescope(SMCT)
For the future MeV Gamma-rayAstronomy
Maybe by a big mission Or by a small satellite
Or by a formation flight
Or by a balloon
T.Takahashi, Astronomy with Radioactivies IV,2003
CdTe telescope• CdTe has a high Compton Efficiency for the energy above 300 keV ( Eff. = 40% at 1MeV for 80 layers , 250 cm2) Compact Compton Telescope for micro/small satellite(important to increase chances of the mission)
25cm
80layers
80 layers of0.5 mm thickCdTe (and/or Si)
Conceptual design of CdTe SMCT
Si
Si
Si
CdTe
CdTe
CdTe
Eff. of MultiCompton
Note: Angular resolution
Large FOV
Polarization
T.Takahashi, Astronomy with Radioactivies IV,2003
Active Pair Telescope (APT)Above 10 MeV, Pair Production is the dominant process
radiation length (r.l.)of CdTe:1.52cm
-> can be used as an active CONVERTER as well as a calorimeter (total r.l. -> 2.6 r.l. for80 layers )
0.5 mm thick CdTe --> 0.03 r.l(same as the conversion foil used in GLAST)
Highly Sensitivedetector below 100 MeV
Fully active pair production telescopeGLAST Gamma-ray below 100 MeV would be absorbed by conversion foil (loose efficiency)
CdTe APT
(Takahashi et al. 2003, SPIE, vol. 4851)
T.Takahashi, Astronomy with Radioactivies IV,2003
Summary• Development of High Resolution CdTe and Si
strips/pixels are in progress.– Pixels, Strips and related technology for CdTe/CZT/Si
are now well in our hands.– ex. Focal plane detector for the super mirror
• New detector concepts– Narrow FOV Compton telescope (SGD) for the NeXT
mission (upto several hundred keV, polarization)– Semiconductor Multi Compton Telescope (SMCT) for
MeV gamma-rays– Active Pair-production Telescope (APT)
• For the demonstration, we will have balloonmissions in 2003-2006.