Double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te
The double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te have been determined from parent-daughter mass differences measured with the Canadian Penning Trap mass spectrometer. The {sup 132}Xe-{sup 129}Xe mass difference, which is precisely known, was also determined to confirm th...
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creator | Scielzo, N. D. Caldwell, S. Savard, G. Sternberg, M. Van Schelt, J. Department of Physics, University of Chicago, Chicago, Illinois 60637 Clark, J. A. Levand, A. F. Sun, T. Deibel, C. M. Joint Institute of Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824 Fallis, J. Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba R3T 2N2 Gulick, S. Lascar, D. Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208 Li, G. Department of Physics, McGill University, Montreal, Quebec H3A 2T8 Mintz, J. Norman, E. B. Department of Nuclear Engineering, University of California, Berkeley, California 94720 Sharma, K. S. |
description | The double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te have been determined from parent-daughter mass differences measured with the Canadian Penning Trap mass spectrometer. The {sup 132}Xe-{sup 129}Xe mass difference, which is precisely known, was also determined to confirm the accuracy of these results. The {sup 130}Te Q value was found to be 2527.01{+-}0.32 keV, which is 3.3 keV lower than the 2003 Atomic Mass Evaluation recommended value and is consistent with another recent Penning trap measurement. The {sup 128}Te and {sup 120}Te Q values were found to be 865.87{+-}1.31 and 1714.81{+-}1.25 keV, respectively. For {sup 120}Te, this reduction in uncertainty of nearly a factor of 8 opens up the possibility of using this isotope for sensitive searches for neutrinoless double-electron capture and electron capture with {beta}{sup +}emission. |
doi_str_mv | 10.1103/PHYSREVC.80.025501 |
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D. ; Caldwell, S. ; Savard, G. ; Sternberg, M. ; Van Schelt, J. ; Department of Physics, University of Chicago, Chicago, Illinois 60637 ; Clark, J. A. ; Levand, A. F. ; Sun, T. ; Deibel, C. M. ; Joint Institute of Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824 ; Fallis, J. ; Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba R3T 2N2 ; Gulick, S. ; Lascar, D. ; Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208 ; Li, G. ; Department of Physics, McGill University, Montreal, Quebec H3A 2T8 ; Mintz, J. ; Norman, E. B. ; Department of Nuclear Engineering, University of California, Berkeley, California 94720 ; Sharma, K. S.</creator><creatorcontrib>Scielzo, N. D. ; Caldwell, S. ; Savard, G. ; Sternberg, M. ; Van Schelt, J. ; Department of Physics, University of Chicago, Chicago, Illinois 60637 ; Clark, J. A. ; Levand, A. F. ; Sun, T. ; Deibel, C. M. ; Joint Institute of Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824 ; Fallis, J. ; Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba R3T 2N2 ; Gulick, S. ; Lascar, D. ; Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208 ; Li, G. ; Department of Physics, McGill University, Montreal, Quebec H3A 2T8 ; Mintz, J. ; Norman, E. B. ; Department of Nuclear Engineering, University of California, Berkeley, California 94720 ; Sharma, K. S.</creatorcontrib><description>The double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te have been determined from parent-daughter mass differences measured with the Canadian Penning Trap mass spectrometer. The {sup 132}Xe-{sup 129}Xe mass difference, which is precisely known, was also determined to confirm the accuracy of these results. The {sup 130}Te Q value was found to be 2527.01{+-}0.32 keV, which is 3.3 keV lower than the 2003 Atomic Mass Evaluation recommended value and is consistent with another recent Penning trap measurement. The {sup 128}Te and {sup 120}Te Q values were found to be 865.87{+-}1.31 and 1714.81{+-}1.25 keV, respectively. For {sup 120}Te, this reduction in uncertainty of nearly a factor of 8 opens up the possibility of using this isotope for sensitive searches for neutrinoless double-electron capture and electron capture with {beta}{sup +}emission.</description><identifier>ISSN: 0556-2813</identifier><identifier>EISSN: 1089-490X</identifier><identifier>DOI: 10.1103/PHYSREVC.80.025501</identifier><language>eng</language><publisher>United States</publisher><subject>DOUBLE BETA DECAY ; ELECTRON CAPTURE ; EMISSION ; EVALUATION ; KEV RANGE ; MASS ; MASS DIFFERENCE ; MASS SPECTROMETERS ; NUCLEAR PHYSICS AND RADIATION PHYSICS ; Q-VALUE ; TELLURIUM 120 ; TELLURIUM 128 ; TELLURIUM 130 ; XENON 129 ; XENON 130 ; XENON 131 ; XENON 131 TARGET ; XENON 132</subject><ispartof>Physical review. 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M.</creatorcontrib><creatorcontrib>Joint Institute of Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824</creatorcontrib><creatorcontrib>Fallis, J.</creatorcontrib><creatorcontrib>Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba R3T 2N2</creatorcontrib><creatorcontrib>Gulick, S.</creatorcontrib><creatorcontrib>Lascar, D.</creatorcontrib><creatorcontrib>Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208</creatorcontrib><creatorcontrib>Li, G.</creatorcontrib><creatorcontrib>Department of Physics, McGill University, Montreal, Quebec H3A 2T8</creatorcontrib><creatorcontrib>Mintz, J.</creatorcontrib><creatorcontrib>Norman, E. B.</creatorcontrib><creatorcontrib>Department of Nuclear Engineering, University of California, Berkeley, California 94720</creatorcontrib><creatorcontrib>Sharma, K. S.</creatorcontrib><title>Double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te</title><title>Physical review. C, Nuclear physics</title><description>The double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te have been determined from parent-daughter mass differences measured with the Canadian Penning Trap mass spectrometer. The {sup 132}Xe-{sup 129}Xe mass difference, which is precisely known, was also determined to confirm the accuracy of these results. The {sup 130}Te Q value was found to be 2527.01{+-}0.32 keV, which is 3.3 keV lower than the 2003 Atomic Mass Evaluation recommended value and is consistent with another recent Penning trap measurement. The {sup 128}Te and {sup 120}Te Q values were found to be 865.87{+-}1.31 and 1714.81{+-}1.25 keV, respectively. For {sup 120}Te, this reduction in uncertainty of nearly a factor of 8 opens up the possibility of using this isotope for sensitive searches for neutrinoless double-electron capture and electron capture with {beta}{sup +}emission.</description><subject>DOUBLE BETA DECAY</subject><subject>ELECTRON CAPTURE</subject><subject>EMISSION</subject><subject>EVALUATION</subject><subject>KEV RANGE</subject><subject>MASS</subject><subject>MASS DIFFERENCE</subject><subject>MASS SPECTROMETERS</subject><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><subject>Q-VALUE</subject><subject>TELLURIUM 120</subject><subject>TELLURIUM 128</subject><subject>TELLURIUM 130</subject><subject>XENON 129</subject><subject>XENON 130</subject><subject>XENON 131</subject><subject>XENON 131 TARGET</subject><subject>XENON 132</subject><issn>0556-2813</issn><issn>1089-490X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNqNissKwjAURIMoWB8_4Crg1tSbxGqy1orufCG6kjSNqJRGSCpI8d99oHtnM5wzg1CHQkgp8P5itl-v4u04FBACiyKgFRRQEJIMJOyqKIAoGhImKK-jhnMXeIXzYYDmE1skmSFlYrx6kNRodcdLfFNZYRy2R1y64ooph8fG9L7AxAdUnv7Ee22h2lFlzrS_3UTdabwZz4h1_nxw-uyNPmmb50b7A6NM8pGQ_L_XE50qQaY</recordid><startdate>20090815</startdate><enddate>20090815</enddate><creator>Scielzo, N. 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B. ; Department of Nuclear Engineering, University of California, Berkeley, California 94720 ; Sharma, K. S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-osti_scitechconnect_212937893</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>DOUBLE BETA DECAY</topic><topic>ELECTRON CAPTURE</topic><topic>EMISSION</topic><topic>EVALUATION</topic><topic>KEV RANGE</topic><topic>MASS</topic><topic>MASS DIFFERENCE</topic><topic>MASS SPECTROMETERS</topic><topic>NUCLEAR PHYSICS AND RADIATION PHYSICS</topic><topic>Q-VALUE</topic><topic>TELLURIUM 120</topic><topic>TELLURIUM 128</topic><topic>TELLURIUM 130</topic><topic>XENON 129</topic><topic>XENON 130</topic><topic>XENON 131</topic><topic>XENON 131 TARGET</topic><topic>XENON 132</topic><toplevel>online_resources</toplevel><creatorcontrib>Scielzo, N. D.</creatorcontrib><creatorcontrib>Caldwell, S.</creatorcontrib><creatorcontrib>Savard, G.</creatorcontrib><creatorcontrib>Sternberg, M.</creatorcontrib><creatorcontrib>Van Schelt, J.</creatorcontrib><creatorcontrib>Department of Physics, University of Chicago, Chicago, Illinois 60637</creatorcontrib><creatorcontrib>Clark, J. A.</creatorcontrib><creatorcontrib>Levand, A. F.</creatorcontrib><creatorcontrib>Sun, T.</creatorcontrib><creatorcontrib>Deibel, C. 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C, Nuclear physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Scielzo, N. D.</au><au>Caldwell, S.</au><au>Savard, G.</au><au>Sternberg, M.</au><au>Van Schelt, J.</au><au>Department of Physics, University of Chicago, Chicago, Illinois 60637</au><au>Clark, J. A.</au><au>Levand, A. F.</au><au>Sun, T.</au><au>Deibel, C. M.</au><au>Joint Institute of Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824</au><au>Fallis, J.</au><au>Department of Physics and Astronomy, University of Manitoba, Winnipeg, Manitoba R3T 2N2</au><au>Gulick, S.</au><au>Lascar, D.</au><au>Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208</au><au>Li, G.</au><au>Department of Physics, McGill University, Montreal, Quebec H3A 2T8</au><au>Mintz, J.</au><au>Norman, E. B.</au><au>Department of Nuclear Engineering, University of California, Berkeley, California 94720</au><au>Sharma, K. S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te</atitle><jtitle>Physical review. C, Nuclear physics</jtitle><date>2009-08-15</date><risdate>2009</risdate><volume>80</volume><issue>2</issue><issn>0556-2813</issn><eissn>1089-490X</eissn><abstract>The double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te have been determined from parent-daughter mass differences measured with the Canadian Penning Trap mass spectrometer. The {sup 132}Xe-{sup 129}Xe mass difference, which is precisely known, was also determined to confirm the accuracy of these results. The {sup 130}Te Q value was found to be 2527.01{+-}0.32 keV, which is 3.3 keV lower than the 2003 Atomic Mass Evaluation recommended value and is consistent with another recent Penning trap measurement. The {sup 128}Te and {sup 120}Te Q values were found to be 865.87{+-}1.31 and 1714.81{+-}1.25 keV, respectively. For {sup 120}Te, this reduction in uncertainty of nearly a factor of 8 opens up the possibility of using this isotope for sensitive searches for neutrinoless double-electron capture and electron capture with {beta}{sup +}emission.</abstract><cop>United States</cop><doi>10.1103/PHYSREVC.80.025501</doi></addata></record> |
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subjects | DOUBLE BETA DECAY ELECTRON CAPTURE EMISSION EVALUATION KEV RANGE MASS MASS DIFFERENCE MASS SPECTROMETERS NUCLEAR PHYSICS AND RADIATION PHYSICS Q-VALUE TELLURIUM 120 TELLURIUM 128 TELLURIUM 130 XENON 129 XENON 130 XENON 131 XENON 131 TARGET XENON 132 |
title | Double-{beta}-decay Q values of {sup 130}Te, {sup 128}Te, and {sup 120}Te |
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