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MeV Gamma Ray Nuclear Astrophysics Yesterday: Science and Observations

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Presentation on theme: "MeV Gamma Ray Nuclear Astrophysics Yesterday: Science and Observations"— Presentation transcript:

1 MeV Gamma Ray Nuclear Astrophysics Yesterday: Science and Observations
Today: Instrumentation (Krause 2004) Steven Boggs UC Berkeley Department of Physics

2 Nuclear Gamma-Rays Atmosphere is opaque at these energies.

3 Gamma-ray interactions
Index of refraction ~1.0000 Penetration ≥ cm into materials Standard mirrors & lenses don’t work

4 Gamma Ray Detectors Solid State Scintillators
good/excellent resolution (<2%) may require cooling finer position resolution more channels/power Liquid Xe NaI, CsI, BGO Scintillators high Z large volume room temperature moderate/poor resolution (3-10%) Si Semiconductor CZT Semiconductor Ge Semiconductor

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6 The radiation environment
The Space Radiation Environment Sun through solar flares: photons, charged particles The radiation environment Radiation belts: Trapped protons (SAA) & resulting activation, electrons Secondaries induced by cosmic-ray interaction with upper atmosphere: Albedo photons, neutrons, electrons, positrons Cosmic rays: Photons Protons (& activation) Alphas Ions Electrons Positrons In space our little detector is exposed to a very unfriendly environment

7 Compton Gamma-Ray Observatory
( ) COMPTEL ( MeV) OSSE (50 keV – 10 MeV) BATSE ( keV) EGRET (20 MeV – 30 GeV)

8 Spectroscopy, no Imaging
“light bucket” Galactic Center Positrons (Purcell et al., 1993)

9 (from P. von Ballmoos)

10 Coded Aperture Imaging
pinhole camera…. with lots of pinholes Good for: point sources photons that stop in the mask (<0.2 MeV)

11 INTErnational Gamma-Ray Astrophysics Laboratory (launched October 2002)
IBIS (15 keV-10 MeV) JEM-X (3-35 keV) E/DE ~ 10, Df ~ 20’ E/DE ~ 500, Df ~ 2º SPI (30 keV-8 MeV) OMC ( nm)

12 IBIS/INTEGRAL ISGRI: 128x128 CdTe array (4x4x2 mm3)
PICsIT: 64x64 CsI array (8.4x8.4x30 mm3)

13 IBIS Galactic Plane Survey
(Bird & Walter 2004)

14 SPI/INTEGRAL 19 Ge detectors

15 SPI Positron Map (Weidenspointner et al., 2008)

16 Compton Gamma-Ray Observatory (1991-2000)
COMPTEL ( MeV) OSSE (50 keV – 10 MeV) BATSE ( keV) EGRET (20 MeV – 30 GeV)

17 COMPTEL - Compton Imaging
cos  = 1+mc2(1/E2-1/E) COMPTEL Detectors D1: 4188 cm2 liq. scint. D2: 8620 cm2 NaI DE: 5-8% (FWHM) DX ~ DY ~ 2 cm (1s) DZ ~ 3 cm (1s) Dt ~ 0.25ns COMPTEL Performance MeV E/DE ~ 9-14 (FWHM) Df ~3º Aeff < 20 cm2 FOV ~ 1str (Schoenfelder et al., 1993, ApJS 86, 657)

18 26Al (1.809 MeV), ~1Myr (Oberlack et al., 1996; Pluschke et al., 2001)

19 Compton Telescopes: Then & Now
ACT Enabling Detectors 1 mm3 resolution DE/E ~ 0.2-1% 10-20% efficiency background rejection polarization 3 decades… CGRO/COMPTEL ~40 cm3 resolution DE/E ~ 10% 0.1% efficiency

20 Overview of the Nuclear Compton Telescope Steven Boggs, UCB
A balloon-borne g-ray spectrometer, polarimeter & imager Steven Boggs, UCB NCT Collaboration: Berkeley, NTHU, NCU, NSPO, NUU, LBNL, CESR

21 Nuclear Compton Telescope Heart of NCT: Cross Strip 3-D GeDs
balloon payload Heart of NCT: Cross Strip 3-D GeDs 37x37 strips 2-mm pitch 15-mm thickness 81000 mm3 volume 1.6 mm3 localization ~2.1-keV noise resolution

22 3D GeD Design (Luke et al. 1992, 1994)

23 Single-Pixel Spectra (56Co)
excellent GeD Spectroscopy plus full 3-D positioning

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25 60Co Laboratory Tests 1.173, MeV 1.173 MeV processed image

26 Next flight, May 2009 northern hemisphere primarily compact objects

27 The 2005 balloon flight from Fort Sumner
Impressions from the NCT 2009 Balloon flight

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29 BGO shield Pre-Amps lN2 dewar

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31 Rotor Differential GPS Solar Panels Electronics Bay Detector CSBF SIP

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34 4D sin  = n  Alternate layers of high/low Z materials ex. W/Si D ~ 25 Å (technological limit) < 1 Å ( keV) ~ 30’ f ~ 10 m

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38 (Suntzeff et al.1992; Diehl & Timmes 1998)
SN 1987A in the LMC ~110-4 M (Suntzeff et al.1992; Diehl & Timmes 1998) Blue supergiant (~20 M, 6 M He core) (Arnett et al., 1989) Spherical models predict 44Ti < 1000 km/s 56Ni mixed out to ~3000 km/s (0.7 keV at 68 keV) (Motizuki & Kumagai 2004)

39 Bragg Scattering 2D sin  = n  Use a crystal to bend (“focus”) the -rays D ~ 1 Å (crystal spacing) < 1 Å ( MeV) ~ 10’ f ~ 60 m

40 Laue Lens: Focusing g-rays
von Ballmoos et al., CESR, Toulouse


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