Measured temperature dependence of scintillation camera signals read out by geiger-Müller mode avalanche photodiodes
We are developing a prototype monolithic scintillation camera with optical sensors on the entrance surface (SES) for use with statistically-estimated depth-of-interaction in a continuous scintillator. We opt to use Geiger-Muller mode avalanche photodiodes (GM-APDs) for the SES camera since they poss...
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description | We are developing a prototype monolithic scintillation camera with optical sensors on the entrance surface (SES) for use with statistically-estimated depth-of-interaction in a continuous scintillator. We opt to use Geiger-Muller mode avalanche photodiodes (GM-APDs) for the SES camera since they possess many desirable properties; for the intended application (SES and PET/MR imaging), they offer a thin attenuation profile and an operational insensitivity to large magnetic fields. However, one issue that must be addressed in using GM-APDs in an RF environment (as in MR scanners) is the thermal dissipation that can occur in this semiconductor material. Signals of GM-APDs are strongly dependent on junction temperature. Consequently, we are developing a temperature-controlled GM-APD-based PET camera whose monitored temperature can be used to dynamically account for the temperature dependence of the output signals. Presently, we aim to characterize the output-signal dependence on temperature and bias for a GM-APD-based scintillation camera. We've examined two GM-APDs, a Zecotek prototype MAPD-3N, and a SensL commercial SPMArray2. The dominant effect of temperature on gain that we observe results from a linear dependence of breakdown voltage on temperature (0.071 V/°C and 0.024 V/°C, respectively); at 2.3 V excess bias (voltage above breakdown) the resulting change in gain with temperature (without adjusting bias voltage) is -8.5% per°C for the MAPD-3N and -1.5 % per °C for the SPMArray2. For fixed excess bias, change in dark current with temperature varied widely, decreasing by 25% to 40% as temperature was changed from 20°C to 10°C and again by 20% to 35% going from 10°C to 0°C. Finally, using two MAPD-3N to read out a pair of 3.5-by-3.5-by-20 mm 3 Zecotek LFS-3 scintillators in coincidence, we observe a decrease from 1.7 nsec to 1.5 nsec in coincidence-time resolution as we lowered temperature from 23°C to 10°C. |
doi_str_mv | 10.1109/NSSMIC.2009.5401995 |
format | Conference Proceeding |
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We opt to use Geiger-Muller mode avalanche photodiodes (GM-APDs) for the SES camera since they possess many desirable properties; for the intended application (SES and PET/MR imaging), they offer a thin attenuation profile and an operational insensitivity to large magnetic fields. However, one issue that must be addressed in using GM-APDs in an RF environment (as in MR scanners) is the thermal dissipation that can occur in this semiconductor material. Signals of GM-APDs are strongly dependent on junction temperature. Consequently, we are developing a temperature-controlled GM-APD-based PET camera whose monitored temperature can be used to dynamically account for the temperature dependence of the output signals. Presently, we aim to characterize the output-signal dependence on temperature and bias for a GM-APD-based scintillation camera. We've examined two GM-APDs, a Zecotek prototype MAPD-3N, and a SensL commercial SPMArray2. The dominant effect of temperature on gain that we observe results from a linear dependence of breakdown voltage on temperature (0.071 V/°C and 0.024 V/°C, respectively); at 2.3 V excess bias (voltage above breakdown) the resulting change in gain with temperature (without adjusting bias voltage) is -8.5% per°C for the MAPD-3N and -1.5 % per °C for the SPMArray2. For fixed excess bias, change in dark current with temperature varied widely, decreasing by 25% to 40% as temperature was changed from 20°C to 10°C and again by 20% to 35% going from 10°C to 0°C. Finally, using two MAPD-3N to read out a pair of 3.5-by-3.5-by-20 mm 3 Zecotek LFS-3 scintillators in coincidence, we observe a decrease from 1.7 nsec to 1.5 nsec in coincidence-time resolution as we lowered temperature from 23°C to 10°C.</description><identifier>ISSN: 1082-3654</identifier><identifier>ISSN: 1095-7863</identifier><identifier>ISBN: 9781424439614</identifier><identifier>ISBN: 1424439612</identifier><identifier>EISSN: 2577-0829</identifier><identifier>EISBN: 9781424439621</identifier><identifier>EISBN: 1424439620</identifier><identifier>DOI: 10.1109/NSSMIC.2009.5401995</identifier><identifier>PMID: 20625461</identifier><language>eng</language><publisher>United States: IEEE</publisher><subject>Avalanche photodiodes ; Breakdown voltage ; Cameras ; Optical sensors ; Optimized production technology ; Positron emission tomography ; Prototypes ; Temperature dependence ; Temperature measurement ; Temperature sensors</subject><ispartof>2009 IEEE Nuclear Science Symposium Conference Record (NSS/MIC), 2009, Vol.2009, p.2662-2665</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/5401995$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,780,784,789,790,2058,27925,54920</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/5401995$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/20625461$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Hunter, W.C.J.</creatorcontrib><creatorcontrib>Miyaoka, R.S.</creatorcontrib><creatorcontrib>MacDonald, L.R.</creatorcontrib><creatorcontrib>Lewellen, T.K.</creatorcontrib><title>Measured temperature dependence of scintillation camera signals read out by geiger-Müller mode avalanche photodiodes</title><title>2009 IEEE Nuclear Science Symposium Conference Record (NSS/MIC)</title><addtitle>NSSMIC</addtitle><addtitle>IEEE Nucl Sci Symp Conf Rec (1997)</addtitle><description>We are developing a prototype monolithic scintillation camera with optical sensors on the entrance surface (SES) for use with statistically-estimated depth-of-interaction in a continuous scintillator. We opt to use Geiger-Muller mode avalanche photodiodes (GM-APDs) for the SES camera since they possess many desirable properties; for the intended application (SES and PET/MR imaging), they offer a thin attenuation profile and an operational insensitivity to large magnetic fields. However, one issue that must be addressed in using GM-APDs in an RF environment (as in MR scanners) is the thermal dissipation that can occur in this semiconductor material. Signals of GM-APDs are strongly dependent on junction temperature. Consequently, we are developing a temperature-controlled GM-APD-based PET camera whose monitored temperature can be used to dynamically account for the temperature dependence of the output signals. Presently, we aim to characterize the output-signal dependence on temperature and bias for a GM-APD-based scintillation camera. We've examined two GM-APDs, a Zecotek prototype MAPD-3N, and a SensL commercial SPMArray2. The dominant effect of temperature on gain that we observe results from a linear dependence of breakdown voltage on temperature (0.071 V/°C and 0.024 V/°C, respectively); at 2.3 V excess bias (voltage above breakdown) the resulting change in gain with temperature (without adjusting bias voltage) is -8.5% per°C for the MAPD-3N and -1.5 % per °C for the SPMArray2. For fixed excess bias, change in dark current with temperature varied widely, decreasing by 25% to 40% as temperature was changed from 20°C to 10°C and again by 20% to 35% going from 10°C to 0°C. Finally, using two MAPD-3N to read out a pair of 3.5-by-3.5-by-20 mm 3 Zecotek LFS-3 scintillators in coincidence, we observe a decrease from 1.7 nsec to 1.5 nsec in coincidence-time resolution as we lowered temperature from 23°C to 10°C.</description><subject>Avalanche photodiodes</subject><subject>Breakdown voltage</subject><subject>Cameras</subject><subject>Optical sensors</subject><subject>Optimized production technology</subject><subject>Positron emission tomography</subject><subject>Prototypes</subject><subject>Temperature dependence</subject><subject>Temperature measurement</subject><subject>Temperature sensors</subject><issn>1082-3654</issn><issn>1095-7863</issn><issn>2577-0829</issn><isbn>9781424439614</isbn><isbn>1424439612</isbn><isbn>9781424439621</isbn><isbn>1424439620</isbn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2009</creationdate><recordtype>conference_proceeding</recordtype><sourceid>6IE</sourceid><sourceid>RIE</sourceid><recordid>eNpVkNlKA0EQRdsNE2O-ICD9AxOr15l-lOASSPQheQ890zVJy2zMIuTffPPHbIgKPhV176mCewmZMZgzBub-dbNZLxdzDmDmSgIzRp2RqYkTJrmUwmjOzsmYqziOIOHm4p_H5CUZs6BHQis5Ijdd9w7AQUh5TUYcNFdSszEZ1mi7oUVHeywbbG0fFuqwwcphlSGtc9plvup9Udje1xXNbBkw2vl9ZYuOtmgdrYeepke6R7_HNlp_fRYFtrSsHVL7YQtbZQekzaHua-eD2N2Sqzwc4_RnTsj26XG7eIlWb8_LxcMq8jzRfSS1BJfnPHaxNshT1DmHRCaGa2ApjwXnkAqrEMFiarVSEIozQiaJDU2ICbk7vW2GtES3a1pf2va4-40fgNkJ8Ij4Z_-ULb4BhShuFA</recordid><startdate>20091024</startdate><enddate>20091024</enddate><creator>Hunter, W.C.J.</creator><creator>Miyaoka, R.S.</creator><creator>MacDonald, L.R.</creator><creator>Lewellen, T.K.</creator><general>IEEE</general><scope>6IE</scope><scope>6IH</scope><scope>CBEJK</scope><scope>RIE</scope><scope>RIO</scope><scope>NPM</scope></search><sort><creationdate>20091024</creationdate><title>Measured temperature dependence of scintillation camera signals read out by geiger-Müller mode avalanche photodiodes</title><author>Hunter, W.C.J. ; Miyaoka, R.S. ; MacDonald, L.R. ; Lewellen, T.K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i286t-4640dff27d769e2be6f2084892601b273220b3a5ee0aeba655010993488a8143</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2009</creationdate><topic>Avalanche photodiodes</topic><topic>Breakdown voltage</topic><topic>Cameras</topic><topic>Optical sensors</topic><topic>Optimized production technology</topic><topic>Positron emission tomography</topic><topic>Prototypes</topic><topic>Temperature dependence</topic><topic>Temperature measurement</topic><topic>Temperature sensors</topic><toplevel>online_resources</toplevel><creatorcontrib>Hunter, W.C.J.</creatorcontrib><creatorcontrib>Miyaoka, R.S.</creatorcontrib><creatorcontrib>MacDonald, L.R.</creatorcontrib><creatorcontrib>Lewellen, T.K.</creatorcontrib><collection>IEEE Electronic Library (IEL) Conference Proceedings</collection><collection>IEEE Proceedings Order Plan (POP) 1998-present by volume</collection><collection>IEEE Xplore All Conference Proceedings</collection><collection>IEEE Electronic Library (IEL)</collection><collection>IEEE Proceedings Order Plans (POP) 1998-present</collection><collection>PubMed</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Hunter, W.C.J.</au><au>Miyaoka, R.S.</au><au>MacDonald, L.R.</au><au>Lewellen, T.K.</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Measured temperature dependence of scintillation camera signals read out by geiger-Müller mode avalanche photodiodes</atitle><btitle>2009 IEEE Nuclear Science Symposium Conference Record (NSS/MIC)</btitle><stitle>NSSMIC</stitle><addtitle>IEEE Nucl Sci Symp Conf Rec (1997)</addtitle><date>2009-10-24</date><risdate>2009</risdate><volume>2009</volume><spage>2662</spage><epage>2665</epage><pages>2662-2665</pages><issn>1082-3654</issn><issn>1095-7863</issn><eissn>2577-0829</eissn><isbn>9781424439614</isbn><isbn>1424439612</isbn><eisbn>9781424439621</eisbn><eisbn>1424439620</eisbn><abstract>We are developing a prototype monolithic scintillation camera with optical sensors on the entrance surface (SES) for use with statistically-estimated depth-of-interaction in a continuous scintillator. We opt to use Geiger-Muller mode avalanche photodiodes (GM-APDs) for the SES camera since they possess many desirable properties; for the intended application (SES and PET/MR imaging), they offer a thin attenuation profile and an operational insensitivity to large magnetic fields. However, one issue that must be addressed in using GM-APDs in an RF environment (as in MR scanners) is the thermal dissipation that can occur in this semiconductor material. Signals of GM-APDs are strongly dependent on junction temperature. Consequently, we are developing a temperature-controlled GM-APD-based PET camera whose monitored temperature can be used to dynamically account for the temperature dependence of the output signals. Presently, we aim to characterize the output-signal dependence on temperature and bias for a GM-APD-based scintillation camera. We've examined two GM-APDs, a Zecotek prototype MAPD-3N, and a SensL commercial SPMArray2. The dominant effect of temperature on gain that we observe results from a linear dependence of breakdown voltage on temperature (0.071 V/°C and 0.024 V/°C, respectively); at 2.3 V excess bias (voltage above breakdown) the resulting change in gain with temperature (without adjusting bias voltage) is -8.5% per°C for the MAPD-3N and -1.5 % per °C for the SPMArray2. For fixed excess bias, change in dark current with temperature varied widely, decreasing by 25% to 40% as temperature was changed from 20°C to 10°C and again by 20% to 35% going from 10°C to 0°C. Finally, using two MAPD-3N to read out a pair of 3.5-by-3.5-by-20 mm 3 Zecotek LFS-3 scintillators in coincidence, we observe a decrease from 1.7 nsec to 1.5 nsec in coincidence-time resolution as we lowered temperature from 23°C to 10°C.</abstract><cop>United States</cop><pub>IEEE</pub><pmid>20625461</pmid><doi>10.1109/NSSMIC.2009.5401995</doi><tpages>4</tpages></addata></record> |
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subjects | Avalanche photodiodes Breakdown voltage Cameras Optical sensors Optimized production technology Positron emission tomography Prototypes Temperature dependence Temperature measurement Temperature sensors |
title | Measured temperature dependence of scintillation camera signals read out by geiger-Müller mode avalanche photodiodes |
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