R. BIanford, P. Chen, T. Kamae, G. Madejski, J. Ng, T. Mizuno, H. Tajima, T. Thurston, L. Barbier, P. Bloser, T. Cline, S. Hunter, A. Harding, J. Krizmanic, J. Mitchell, R. Streitmatter, J. Tueller, E. Groth, R. Fernholz, D. Marlow, G. Bogaert, S. Gunji, H. Sakurai, Y. Saito, T. Takahashi, J. Kataoka, N. Kawai, Y. Fukazawa, P. Carlson, W. Klamra, M. Pearce, C. Bjornsson, C. Fransson, S. Larsson, F. Ryde
{"title":"大面积球载偏振伽马射线观测仪","authors":"R. BIanford, P. Chen, T. Kamae, G. Madejski, J. Ng, T. Mizuno, H. Tajima, T. Thurston, L. Barbier, P. Bloser, T. Cline, S. Hunter, A. Harding, J. Krizmanic, J. Mitchell, R. Streitmatter, J. Tueller, E. Groth, R. Fernholz, D. Marlow, G. Bogaert, S. Gunji, H. Sakurai, Y. Saito, T. Takahashi, J. Kataoka, N. Kawai, Y. Fukazawa, P. Carlson, W. Klamra, M. Pearce, C. Bjornsson, C. Fransson, S. Larsson, F. Ryde","doi":"10.1109/NSSMIC.2003.1352208","DOIUrl":null,"url":null,"abstract":"We are developing a new balloon-borne instrument (PoGO), to measure polarization of soft gamma rays (25-200 keV) using asymmetry in azimuth angle distribution of Compton scattering. PoGO will detect 10% polarization in 100mCrab sources in a 6-8 hour observation and bring a new dimension to studies on gamma ray emission/transportation mechanism in pulsars, AGNs, black hole binaries, and neutron star surface. The concept is an adaptation to polarization measurements of well-type phoswich counter technology used in balloon-borne experiments (Welcome-1) and AstroE2 Hard X-ray Detector. PoGO consists of close-packed array of 397 hexagonal well-type phoswich counters. Each unit is composed of a long thin tube (well) of slow plastic scintillator, a solid rod of fast plastic scintillator, and a short BGO at the base. A photomultiplier coupled to the end of the BGO detects light from all 3 scintillators. The rods with decay times < 10 ns, are used as the active elements; while the wells and BGOs, with decay times /spl sim/ 250 ns are used as active anti-coincidence. The fast and slow signals are separated out electronically. When gamma rays entering the field-of-view (fwhm /spl sim/3deg/sup 2/) strike a fast scintillator, some are Compton scattered. A fraction of the scattered photons are absorbed in another rod (or undergo a second scatter). A valid event requires one clean fast signal of pulse-height compatible with photo-absorption (> 20 keV) and one or more compatible with Compton scattering (< 10 keV). Studies based on EGS4 (with polarization features) and Geant4 predict excellent background rejection and high sensitivity.","PeriodicalId":186175,"journal":{"name":"2003 IEEE Nuclear Science Symposium. Conference Record (IEEE Cat. No.03CH37515)","volume":"13 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2003-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":"{\"title\":\"Large-area balloon-borne polarized gamma ray observer (PoGO)\",\"authors\":\"R. BIanford, P. Chen, T. Kamae, G. Madejski, J. Ng, T. Mizuno, H. Tajima, T. Thurston, L. Barbier, P. Bloser, T. Cline, S. Hunter, A. Harding, J. Krizmanic, J. Mitchell, R. Streitmatter, J. Tueller, E. Groth, R. Fernholz, D. Marlow, G. Bogaert, S. Gunji, H. Sakurai, Y. Saito, T. Takahashi, J. Kataoka, N. Kawai, Y. Fukazawa, P. Carlson, W. Klamra, M. Pearce, C. Bjornsson, C. Fransson, S. Larsson, F. Ryde\",\"doi\":\"10.1109/NSSMIC.2003.1352208\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We are developing a new balloon-borne instrument (PoGO), to measure polarization of soft gamma rays (25-200 keV) using asymmetry in azimuth angle distribution of Compton scattering. PoGO will detect 10% polarization in 100mCrab sources in a 6-8 hour observation and bring a new dimension to studies on gamma ray emission/transportation mechanism in pulsars, AGNs, black hole binaries, and neutron star surface. The concept is an adaptation to polarization measurements of well-type phoswich counter technology used in balloon-borne experiments (Welcome-1) and AstroE2 Hard X-ray Detector. PoGO consists of close-packed array of 397 hexagonal well-type phoswich counters. Each unit is composed of a long thin tube (well) of slow plastic scintillator, a solid rod of fast plastic scintillator, and a short BGO at the base. A photomultiplier coupled to the end of the BGO detects light from all 3 scintillators. The rods with decay times < 10 ns, are used as the active elements; while the wells and BGOs, with decay times /spl sim/ 250 ns are used as active anti-coincidence. The fast and slow signals are separated out electronically. When gamma rays entering the field-of-view (fwhm /spl sim/3deg/sup 2/) strike a fast scintillator, some are Compton scattered. A fraction of the scattered photons are absorbed in another rod (or undergo a second scatter). A valid event requires one clean fast signal of pulse-height compatible with photo-absorption (> 20 keV) and one or more compatible with Compton scattering (< 10 keV). 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Large-area balloon-borne polarized gamma ray observer (PoGO)
We are developing a new balloon-borne instrument (PoGO), to measure polarization of soft gamma rays (25-200 keV) using asymmetry in azimuth angle distribution of Compton scattering. PoGO will detect 10% polarization in 100mCrab sources in a 6-8 hour observation and bring a new dimension to studies on gamma ray emission/transportation mechanism in pulsars, AGNs, black hole binaries, and neutron star surface. The concept is an adaptation to polarization measurements of well-type phoswich counter technology used in balloon-borne experiments (Welcome-1) and AstroE2 Hard X-ray Detector. PoGO consists of close-packed array of 397 hexagonal well-type phoswich counters. Each unit is composed of a long thin tube (well) of slow plastic scintillator, a solid rod of fast plastic scintillator, and a short BGO at the base. A photomultiplier coupled to the end of the BGO detects light from all 3 scintillators. The rods with decay times < 10 ns, are used as the active elements; while the wells and BGOs, with decay times /spl sim/ 250 ns are used as active anti-coincidence. The fast and slow signals are separated out electronically. When gamma rays entering the field-of-view (fwhm /spl sim/3deg/sup 2/) strike a fast scintillator, some are Compton scattered. A fraction of the scattered photons are absorbed in another rod (or undergo a second scatter). A valid event requires one clean fast signal of pulse-height compatible with photo-absorption (> 20 keV) and one or more compatible with Compton scattering (< 10 keV). Studies based on EGS4 (with polarization features) and Geant4 predict excellent background rejection and high sensitivity.