Segmented Ge detector rejection of internal beta activity produced by neutron irradiation

Future Ge spectrometers flown in space to observe cosmic gamma-ray sources will incorporate segmented detectors to reduce the background from radioactivity produced by energetic particle reactions. To demonstrate the effectiveness of a segmented Ge detector in rejecting background events due to the...

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Veröffentlicht in:IEEE transactions on nuclear science 1991-04, Vol.38 (2), p.218-220
Hauptverfasser: Varnell, L.S., Callas, J.L., Mahoney, W.A., Pehl, R.H., Landis, D.A., Luke, P.N., Madden, N.W.
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container_end_page 220
container_issue 2
container_start_page 218
container_title IEEE transactions on nuclear science
container_volume 38
creator Varnell, L.S.
Callas, J.L.
Mahoney, W.A.
Pehl, R.H.
Landis, D.A.
Luke, P.N.
Madden, N.W.
description Future Ge spectrometers flown in space to observe cosmic gamma-ray sources will incorporate segmented detectors to reduce the background from radioactivity produced by energetic particle reactions. To demonstrate the effectiveness of a segmented Ge detector in rejecting background events due to the beta decay of internal radioactivity, a laboratory experiment has been carried out in which radioactivity was produced in the detector by neutron irradiation. A /sup 252/Cf source of neutrons was used to produce, by neutron capture on /sup 74/Ge (36.5% of natural Ge) in the detector itself, /sup 75/Ge (t/sub 1/2/=82.78 min), which decays by beta emission with a maximum electron kinetic energy of 1188 keV. By requiring that an ionizing event deposit energy in two or more of the five segments of the detector, each about 1-cm thick, the beta particles, which have a range of about 1-mm, are rejected, while most external gamma rays incident on the detector are counted.< >
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To demonstrate the effectiveness of a segmented Ge detector in rejecting background events due to the beta decay of internal radioactivity, a laboratory experiment has been carried out in which radioactivity was produced in the detector by neutron irradiation. A /sup 252/Cf source of neutrons was used to produce, by neutron capture on /sup 74/Ge (36.5% of natural Ge) in the detector itself, /sup 75/Ge (t/sub 1/2/=82.78 min), which decays by beta emission with a maximum electron kinetic energy of 1188 keV. 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To demonstrate the effectiveness of a segmented Ge detector in rejecting background events due to the beta decay of internal radioactivity, a laboratory experiment has been carried out in which radioactivity was produced in the detector by neutron irradiation. A /sup 252/Cf source of neutrons was used to produce, by neutron capture on /sup 74/Ge (36.5% of natural Ge) in the detector itself, /sup 75/Ge (t/sub 1/2/=82.78 min), which decays by beta emission with a maximum electron kinetic energy of 1188 keV. By requiring that an ionizing event deposit energy in two or more of the five segments of the detector, each about 1-cm thick, the beta particles, which have a range of about 1-mm, are rejected, while most external gamma rays incident on the detector are counted.&lt; &gt;</description><subject>440200 - Radiation Effects on Instrument Components, Instruments, or Electronic Systems</subject><subject>ACTINIDE ISOTOPES</subject><subject>ACTINIDE NUCLEI</subject><subject>ALPHA DECAY RADIOISOTOPES</subject><subject>BACKGROUND RADIATION</subject><subject>BARYONS</subject><subject>BETA DECAY</subject><subject>BETA DECAY RADIOISOTOPES</subject><subject>Beta rays</subject><subject>BETA-MINUS DECAY RADIOISOTOPES</subject><subject>CALIFORNIUM 252</subject><subject>CALIFORNIUM ISOTOPES</subject><subject>COSMIC GAMMA SOURCES</subject><subject>COSMIC RAY SOURCES</subject><subject>DECAY</subject><subject>Electron emission</subject><subject>ELEMENTARY PARTICLES</subject><subject>Energy capture</subject><subject>EVEN-EVEN NUCLEI</subject><subject>EVEN-ODD NUCLEI</subject><subject>Event detection</subject><subject>Exact sciences and technology</subject><subject>FERMIONS</subject><subject>Gamma ray detection</subject><subject>Gamma ray detectors</subject><subject>GE SEMICONDUCTOR DETECTORS</subject><subject>GERMANIUM 74</subject><subject>GERMANIUM 75</subject><subject>GERMANIUM ISOTOPES</subject><subject>HADRONS</subject><subject>HEAVY NUCLEI</subject><subject>HOURS LIVING RADIOISOTOPES</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>Instruments, apparatus, components and techniques common to several branches of physics and astronomy</subject><subject>INTERMEDIATE MASS NUCLEI</subject><subject>INTERNAL CONVERSION RADIOISOTOPES</subject><subject>IRRADIATION</subject><subject>ISOMERIC TRANSITION ISOTOPES</subject><subject>ISOTOPES</subject><subject>Kinetic energy</subject><subject>Laboratories</subject><subject>MEASURING INSTRUMENTS</subject><subject>NEUTRONS</subject><subject>NUCLEAR DECAY</subject><subject>NUCLEI</subject><subject>NUCLEONS</subject><subject>Other topics in instruments, apparatus, components and techniques common to several branches of physics and astronomy</subject><subject>Physics</subject><subject>RADIATION DETECTORS</subject><subject>RADIATION EFFECTS</subject><subject>RADIATIONS</subject><subject>RADIOISOTOPES</subject><subject>SECONDS LIVING RADIO</subject><subject>SEMICONDUCTOR DETECTORS</subject><subject>SPACE FLIGHT</subject><subject>Spacecraft Instrumentation</subject><subject>Spectroscopy</subject><subject>SPONTANEOUS FISSION RADIOISOTOPES</subject><subject>STABLE ISOTOPES</subject><subject>YEARS LIVING RADIOISOTOPES</subject><issn>0018-9499</issn><issn>1558-1578</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1991</creationdate><recordtype>article</recordtype><sourceid>CYI</sourceid><recordid>eNqFkb1rHDEQxUWIwRfbhduQQoQQSLG2vuZOKo1JnIAhRewildBqZxOZPa0j6QL332eOPdymkkbze0_zGMYupbiSUrhrpa-Udcq5V2wlAWwnYWNfs5UQ0nbOOHfK3tT6RKUBASv28wf-2mJuOPA75AM2jG0uvOATXdKc-TzyRO2Sw8R7bIEHev-b2p4_l3nYRRL2e55x1wrRqZQwpHBQnrOTMUwVL47nGXv88vnh9mt3__3u2-3NfRe1hdaFGORoB6V6sGHoh_UwumiVAaMIMFKOIJ0UMq4B-7WSWkXVB0MlSIHrUZ-x94vvXFvyNSaK8DvOOVMAD8IYrYGgjwtEQ__ZYW1-m2rEaQoZ5131yoIF7ez_QZrLbdyGwE8LGMtca8HRP5e0DWXvpfCHVXil_bIKYj8cTUONYRpLyDHVFwEYvbEgCHu3YDnU4HMr1UtH2QWtEA4ub5d2QsQX8fGLfyWTmLs</recordid><startdate>19910401</startdate><enddate>19910401</enddate><creator>Varnell, L.S.</creator><creator>Callas, J.L.</creator><creator>Mahoney, W.A.</creator><creator>Pehl, R.H.</creator><creator>Landis, D.A.</creator><creator>Luke, P.N.</creator><creator>Madden, N.W.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>CYE</scope><scope>CYI</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>KR7</scope><scope>L7M</scope><scope>7U5</scope><scope>OTOTI</scope></search><sort><creationdate>19910401</creationdate><title>Segmented Ge detector rejection of internal beta activity produced by neutron irradiation</title><author>Varnell, L.S. ; 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To demonstrate the effectiveness of a segmented Ge detector in rejecting background events due to the beta decay of internal radioactivity, a laboratory experiment has been carried out in which radioactivity was produced in the detector by neutron irradiation. A /sup 252/Cf source of neutrons was used to produce, by neutron capture on /sup 74/Ge (36.5% of natural Ge) in the detector itself, /sup 75/Ge (t/sub 1/2/=82.78 min), which decays by beta emission with a maximum electron kinetic energy of 1188 keV. By requiring that an ionizing event deposit energy in two or more of the five segments of the detector, each about 1-cm thick, the beta particles, which have a range of about 1-mm, are rejected, while most external gamma rays incident on the detector are counted.&lt; &gt;</abstract><cop>Legacy CDMS</cop><pub>IEEE</pub><doi>10.1109/23.289299</doi><tpages>3</tpages></addata></record>
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subjects 440200 - Radiation Effects on Instrument Components, Instruments, or Electronic Systems
ACTINIDE ISOTOPES
ACTINIDE NUCLEI
ALPHA DECAY RADIOISOTOPES
BACKGROUND RADIATION
BARYONS
BETA DECAY
BETA DECAY RADIOISOTOPES
Beta rays
BETA-MINUS DECAY RADIOISOTOPES
CALIFORNIUM 252
CALIFORNIUM ISOTOPES
COSMIC GAMMA SOURCES
COSMIC RAY SOURCES
DECAY
Electron emission
ELEMENTARY PARTICLES
Energy capture
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
Event detection
Exact sciences and technology
FERMIONS
Gamma ray detection
Gamma ray detectors
GE SEMICONDUCTOR DETECTORS
GERMANIUM 74
GERMANIUM 75
GERMANIUM ISOTOPES
HADRONS
HEAVY NUCLEI
HOURS LIVING RADIOISOTOPES
INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY
Instruments, apparatus, components and techniques common to several branches of physics and astronomy
INTERMEDIATE MASS NUCLEI
INTERNAL CONVERSION RADIOISOTOPES
IRRADIATION
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
Kinetic energy
Laboratories
MEASURING INSTRUMENTS
NEUTRONS
NUCLEAR DECAY
NUCLEI
NUCLEONS
Other topics in instruments, apparatus, components and techniques common to several branches of physics and astronomy
Physics
RADIATION DETECTORS
RADIATION EFFECTS
RADIATIONS
RADIOISOTOPES
SECONDS LIVING RADIO
SEMICONDUCTOR DETECTORS
SPACE FLIGHT
Spacecraft Instrumentation
Spectroscopy
SPONTANEOUS FISSION RADIOISOTOPES
STABLE ISOTOPES
YEARS LIVING RADIOISOTOPES
title Segmented Ge detector rejection of internal beta activity produced by neutron irradiation
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