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Weak decays of {sub {lambda}}{sup 4}He
We measured the lifetime and the mesonic and nonmesonic decay rates of the {sub {lambda}}{sup 4}He hypernucleus. The hypernuclei were created using a 750 MeV/c momentum K{sup -} beam on a liquid {sup 4}He target by the reaction {sup 4}He (K{sup -},{pi}{sup -}){sub {lambda}}{sup 4}He. The {sub {lambd...
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Published in: | Physical review. C, Nuclear physics Nuclear physics, 2007-09, Vol.76 (3) |
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container_title | Physical review. C, Nuclear physics |
container_volume | 76 |
creator | Parker, J. D. Athanas, M. J. Barnes, P. D. Diebold, G. Franklin, G. B. Quinn, B. Rozon, F. Schumacher, R. A. Sukaton, I. Zeps, V. J. Bart, S. Chrien, R. Pile, P. Sawafta, R. Sutter, R. Bassalleck, B. Johnston, K. Stearns, R. Szymanski, J. J. |
description | We measured the lifetime and the mesonic and nonmesonic decay rates of the {sub {lambda}}{sup 4}He hypernucleus. The hypernuclei were created using a 750 MeV/c momentum K{sup -} beam on a liquid {sup 4}He target by the reaction {sup 4}He (K{sup -},{pi}{sup -}){sub {lambda}}{sup 4}He. The {sub {lambda}}{sup 4}He lifetime was directly measured using protons from {lambda}p{yields}np nonmesonic decay (also referred to as proton-stimulated decay) and was found to have a value of {tau}=245{+-}24 ps. The mesonic decay rates were determined from the observed numbers of {pi}{sup -}'s and {pi}{sup circle}'s as {gamma}{sub {pi}{sup -}}/{gamma}{sub tot}=0.270{+-}0.024 and {gamma}{sub {pi}}/{gamma}{sub tot}=0.564{+-}0.036, respectively, and the values of the proton- and neutron-stimulated decay rates were extracted as {gamma}{sub p}/{gamma}{sub tot}=0.169{+-}0.019 and {gamma}{sub n}/{gamma}{sub tot}{ |
doi_str_mv | 10.1103/PHYSREVC.76.035501 |
format | article |
fullrecord | <record><control><sourceid>osti</sourceid><recordid>TN_cdi_osti_scitechconnect_21064378</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>21064378</sourcerecordid><originalsourceid>FETCH-osti_scitechconnect_210643783</originalsourceid><addsrcrecordid>eNpjYJAyNNAzNDQw1g_wiAwOcg1z1jM30zMwNjU1MGRi4DQ0sLDUNbE0iGBh4DQwNTXTNbIwNOZg4CouzjIAAmNjM04GtfDUxGyFlNTkxMpihfw0heri0iSF6pzE3KSUxNpaIK9AwaTWI5WHgTUtMac4lRdKczMou7mGOHvo5heXZMYXJ2eWpCZnJOfn5aUml8QbGRqYmRibWxgTpwoAaYA3Cg</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Weak decays of {sub {lambda}}{sup 4}He</title><source>American Physical Society:Jisc Collections:APS Read and Publish 2023-2025 (reading list)</source><creator>Parker, J. D. ; Athanas, M. J. ; Barnes, P. D. ; Diebold, G. ; Franklin, G. B. ; Quinn, B. ; Rozon, F. ; Schumacher, R. A. ; Sukaton, I. ; Zeps, V. J. ; Bart, S. ; Chrien, R. ; Pile, P. ; Sawafta, R. ; Sutter, R. ; Bassalleck, B. ; Johnston, K. ; Stearns, R. ; Szymanski, J. J.</creator><creatorcontrib>Parker, J. D. ; Athanas, M. J. ; Barnes, P. D. ; Diebold, G. ; Franklin, G. B. ; Quinn, B. ; Rozon, F. ; Schumacher, R. A. ; Sukaton, I. ; Zeps, V. J. ; Bart, S. ; Chrien, R. ; Pile, P. ; Sawafta, R. ; Sutter, R. ; Bassalleck, B. ; Johnston, K. ; Stearns, R. ; Szymanski, J. J.</creatorcontrib><description>We measured the lifetime and the mesonic and nonmesonic decay rates of the {sub {lambda}}{sup 4}He hypernucleus. The hypernuclei were created using a 750 MeV/c momentum K{sup -} beam on a liquid {sup 4}He target by the reaction {sup 4}He (K{sup -},{pi}{sup -}){sub {lambda}}{sup 4}He. The {sub {lambda}}{sup 4}He lifetime was directly measured using protons from {lambda}p{yields}np nonmesonic decay (also referred to as proton-stimulated decay) and was found to have a value of {tau}=245{+-}24 ps. The mesonic decay rates were determined from the observed numbers of {pi}{sup -}'s and {pi}{sup circle}'s as {gamma}{sub {pi}{sup -}}/{gamma}{sub tot}=0.270{+-}0.024 and {gamma}{sub {pi}}/{gamma}{sub tot}=0.564{+-}0.036, respectively, and the values of the proton- and neutron-stimulated decay rates were extracted as {gamma}{sub p}/{gamma}{sub tot}=0.169{+-}0.019 and {gamma}{sub n}/{gamma}{sub tot}{<=}0.032 (95% CL), respectively. The effects of final-state interactions and possible three-body {lambda}NN decay contributions were studied in the context of a simple model of nucleon-stimulated decay. Nucleon-nucleon coincidence events were observed and were used in the determination of the nonmesonic branching fractions. The implications of the results of this analysis were considered for the empirical {delta}I=(1/2) rule and the decay rates of the {sub {lambda}}{sup 4}H hypernucleus.</description><identifier>ISSN: 0556-2813</identifier><identifier>EISSN: 1089-490X</identifier><identifier>DOI: 10.1103/PHYSREVC.76.035501</identifier><language>eng</language><publisher>United States</publisher><subject>BRANCHING RATIO ; FINAL-STATE INTERACTIONS ; HELIUM 4 ; HELIUM 4 TARGET ; HYPERNUCLEI ; KAON MINUS REACTIONS ; LAMBDA BARYONS ; LIFETIME ; MEV RANGE ; NEUTRONS ; NUCLEAR DECAY ; NUCLEAR PHYSICS AND RADIATION PHYSICS ; PARTICLE DECAY ; PIONS MINUS ; PROTONS ; THREE-BODY PROBLEM</subject><ispartof>Physical review. C, Nuclear physics, 2007-09, Vol.76 (3)</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27901,27902</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/21064378$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Parker, J. D.</creatorcontrib><creatorcontrib>Athanas, M. J.</creatorcontrib><creatorcontrib>Barnes, P. D.</creatorcontrib><creatorcontrib>Diebold, G.</creatorcontrib><creatorcontrib>Franklin, G. B.</creatorcontrib><creatorcontrib>Quinn, B.</creatorcontrib><creatorcontrib>Rozon, F.</creatorcontrib><creatorcontrib>Schumacher, R. A.</creatorcontrib><creatorcontrib>Sukaton, I.</creatorcontrib><creatorcontrib>Zeps, V. J.</creatorcontrib><creatorcontrib>Bart, S.</creatorcontrib><creatorcontrib>Chrien, R.</creatorcontrib><creatorcontrib>Pile, P.</creatorcontrib><creatorcontrib>Sawafta, R.</creatorcontrib><creatorcontrib>Sutter, R.</creatorcontrib><creatorcontrib>Bassalleck, B.</creatorcontrib><creatorcontrib>Johnston, K.</creatorcontrib><creatorcontrib>Stearns, R.</creatorcontrib><creatorcontrib>Szymanski, J. J.</creatorcontrib><title>Weak decays of {sub {lambda}}{sup 4}He</title><title>Physical review. C, Nuclear physics</title><description>We measured the lifetime and the mesonic and nonmesonic decay rates of the {sub {lambda}}{sup 4}He hypernucleus. The hypernuclei were created using a 750 MeV/c momentum K{sup -} beam on a liquid {sup 4}He target by the reaction {sup 4}He (K{sup -},{pi}{sup -}){sub {lambda}}{sup 4}He. The {sub {lambda}}{sup 4}He lifetime was directly measured using protons from {lambda}p{yields}np nonmesonic decay (also referred to as proton-stimulated decay) and was found to have a value of {tau}=245{+-}24 ps. The mesonic decay rates were determined from the observed numbers of {pi}{sup -}'s and {pi}{sup circle}'s as {gamma}{sub {pi}{sup -}}/{gamma}{sub tot}=0.270{+-}0.024 and {gamma}{sub {pi}}/{gamma}{sub tot}=0.564{+-}0.036, respectively, and the values of the proton- and neutron-stimulated decay rates were extracted as {gamma}{sub p}/{gamma}{sub tot}=0.169{+-}0.019 and {gamma}{sub n}/{gamma}{sub tot}{<=}0.032 (95% CL), respectively. The effects of final-state interactions and possible three-body {lambda}NN decay contributions were studied in the context of a simple model of nucleon-stimulated decay. Nucleon-nucleon coincidence events were observed and were used in the determination of the nonmesonic branching fractions. The implications of the results of this analysis were considered for the empirical {delta}I=(1/2) rule and the decay rates of the {sub {lambda}}{sup 4}H hypernucleus.</description><subject>BRANCHING RATIO</subject><subject>FINAL-STATE INTERACTIONS</subject><subject>HELIUM 4</subject><subject>HELIUM 4 TARGET</subject><subject>HYPERNUCLEI</subject><subject>KAON MINUS REACTIONS</subject><subject>LAMBDA BARYONS</subject><subject>LIFETIME</subject><subject>MEV RANGE</subject><subject>NEUTRONS</subject><subject>NUCLEAR DECAY</subject><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><subject>PARTICLE DECAY</subject><subject>PIONS MINUS</subject><subject>PROTONS</subject><subject>THREE-BODY PROBLEM</subject><issn>0556-2813</issn><issn>1089-490X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><recordid>eNpjYJAyNNAzNDQw1g_wiAwOcg1z1jM30zMwNjU1MGRi4DQ0sLDUNbE0iGBh4DQwNTXTNbIwNOZg4CouzjIAAmNjM04GtfDUxGyFlNTkxMpihfw0heri0iSF6pzE3KSUxNpaIK9AwaTWI5WHgTUtMac4lRdKczMou7mGOHvo5heXZMYXJ2eWpCZnJOfn5aUml8QbGRqYmRibWxgTpwoAaYA3Cg</recordid><startdate>20070915</startdate><enddate>20070915</enddate><creator>Parker, J. 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J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-osti_scitechconnect_210643783</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>BRANCHING RATIO</topic><topic>FINAL-STATE INTERACTIONS</topic><topic>HELIUM 4</topic><topic>HELIUM 4 TARGET</topic><topic>HYPERNUCLEI</topic><topic>KAON MINUS REACTIONS</topic><topic>LAMBDA BARYONS</topic><topic>LIFETIME</topic><topic>MEV RANGE</topic><topic>NEUTRONS</topic><topic>NUCLEAR DECAY</topic><topic>NUCLEAR PHYSICS AND RADIATION PHYSICS</topic><topic>PARTICLE DECAY</topic><topic>PIONS MINUS</topic><topic>PROTONS</topic><topic>THREE-BODY PROBLEM</topic><toplevel>online_resources</toplevel><creatorcontrib>Parker, J. D.</creatorcontrib><creatorcontrib>Athanas, M. J.</creatorcontrib><creatorcontrib>Barnes, P. D.</creatorcontrib><creatorcontrib>Diebold, G.</creatorcontrib><creatorcontrib>Franklin, G. B.</creatorcontrib><creatorcontrib>Quinn, B.</creatorcontrib><creatorcontrib>Rozon, F.</creatorcontrib><creatorcontrib>Schumacher, R. A.</creatorcontrib><creatorcontrib>Sukaton, I.</creatorcontrib><creatorcontrib>Zeps, V. J.</creatorcontrib><creatorcontrib>Bart, S.</creatorcontrib><creatorcontrib>Chrien, R.</creatorcontrib><creatorcontrib>Pile, P.</creatorcontrib><creatorcontrib>Sawafta, R.</creatorcontrib><creatorcontrib>Sutter, R.</creatorcontrib><creatorcontrib>Bassalleck, B.</creatorcontrib><creatorcontrib>Johnston, K.</creatorcontrib><creatorcontrib>Stearns, R.</creatorcontrib><creatorcontrib>Szymanski, J. J.</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Physical review. C, Nuclear physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Parker, J. D.</au><au>Athanas, M. J.</au><au>Barnes, P. D.</au><au>Diebold, G.</au><au>Franklin, G. B.</au><au>Quinn, B.</au><au>Rozon, F.</au><au>Schumacher, R. A.</au><au>Sukaton, I.</au><au>Zeps, V. J.</au><au>Bart, S.</au><au>Chrien, R.</au><au>Pile, P.</au><au>Sawafta, R.</au><au>Sutter, R.</au><au>Bassalleck, B.</au><au>Johnston, K.</au><au>Stearns, R.</au><au>Szymanski, J. J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Weak decays of {sub {lambda}}{sup 4}He</atitle><jtitle>Physical review. C, Nuclear physics</jtitle><date>2007-09-15</date><risdate>2007</risdate><volume>76</volume><issue>3</issue><issn>0556-2813</issn><eissn>1089-490X</eissn><abstract>We measured the lifetime and the mesonic and nonmesonic decay rates of the {sub {lambda}}{sup 4}He hypernucleus. The hypernuclei were created using a 750 MeV/c momentum K{sup -} beam on a liquid {sup 4}He target by the reaction {sup 4}He (K{sup -},{pi}{sup -}){sub {lambda}}{sup 4}He. The {sub {lambda}}{sup 4}He lifetime was directly measured using protons from {lambda}p{yields}np nonmesonic decay (also referred to as proton-stimulated decay) and was found to have a value of {tau}=245{+-}24 ps. The mesonic decay rates were determined from the observed numbers of {pi}{sup -}'s and {pi}{sup circle}'s as {gamma}{sub {pi}{sup -}}/{gamma}{sub tot}=0.270{+-}0.024 and {gamma}{sub {pi}}/{gamma}{sub tot}=0.564{+-}0.036, respectively, and the values of the proton- and neutron-stimulated decay rates were extracted as {gamma}{sub p}/{gamma}{sub tot}=0.169{+-}0.019 and {gamma}{sub n}/{gamma}{sub tot}{<=}0.032 (95% CL), respectively. The effects of final-state interactions and possible three-body {lambda}NN decay contributions were studied in the context of a simple model of nucleon-stimulated decay. Nucleon-nucleon coincidence events were observed and were used in the determination of the nonmesonic branching fractions. The implications of the results of this analysis were considered for the empirical {delta}I=(1/2) rule and the decay rates of the {sub {lambda}}{sup 4}H hypernucleus.</abstract><cop>United States</cop><doi>10.1103/PHYSREVC.76.035501</doi></addata></record> |
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subjects | BRANCHING RATIO FINAL-STATE INTERACTIONS HELIUM 4 HELIUM 4 TARGET HYPERNUCLEI KAON MINUS REACTIONS LAMBDA BARYONS LIFETIME MEV RANGE NEUTRONS NUCLEAR DECAY NUCLEAR PHYSICS AND RADIATION PHYSICS PARTICLE DECAY PIONS MINUS PROTONS THREE-BODY PROBLEM |
title | Weak decays of {sub {lambda}}{sup 4}He |
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