Study of electron-neutrino-electron elastic scattering at LAMPF
Neutrino-electron elastic scattering was observed with a 15-ton fine-grained tracking calorimeter exposed to electron neutrinos from muon decay at rest. The measured [nu][sub [ital e]e][sup [minus]][r arrow][nu][sub [ital e]e][sup [minus]] elastic scattering rate of 236[plus minus]35 events yields t...
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| Veröffentlicht in: | Physical review. D, Particles and fields Particles and fields, 1993, Vol.47 (1), p.11-28 |
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| creator | ALLEN, R. C CHEN, H. H BURMAN, R. L CARLINI, R. D COCHRAN, D. R. F FRANK, J. S PIASETZKY, E SANDBERG, V. D KRAKAUER, D. A TALAGA, R. L DOE, P. J HAUSAMMANN, R LEE, W. P LU, X. Q MHALER, H. J POTTER, M. E WANG, K. C BOWLES, T. J |
| description | Neutrino-electron elastic scattering was observed with a 15-ton fine-grained tracking calorimeter exposed to electron neutrinos from muon decay at rest. The measured [nu][sub [ital e]e][sup [minus]][r arrow][nu][sub [ital e]e][sup [minus]] elastic scattering rate of 236[plus minus]35 events yields the total elastic scattering cross section 10.0[plus minus]1.5(stat)[plus minus]0.9(syst)[times]10[sup [minus]45] cm[sup 2][times][[ital E][sub [nu]] (MeV)], and a model-independent measurement of the strength of the destructive interference between the charged and neutral currents, [ital I]=[minus]1.07[plus minus]0.21, that agrees well with the standard model (SM) prediction [ital I]=[minus]1.08. The agreement between the measured electroweak parameters and SM expectations is used to place limits on neutrino properties, such as neutrino flavor-changing neutral currents and neutrino electromagnetic moments. Limits are placed on the masses of new bosons that interact with leptons: for a neutral tensor boson, [ital M][sub [ital T]][gt]105 GeV; for a neutral (pseudo)scalar boson, [ital M][sub [ital P],][ital S][gt]47 GeV; for a charged Higgs boson, [ital M][sub [chi]][sup +][gt]87 GeV; and for a purely left-handed charged (neutral) vector boson, [ital M][sub [ital x]][gt]239 (119) GeV. |
| doi_str_mv | 10.1103/PhysRevD.47.11 |
| format | Article |
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C ; CHEN, H. H ; BURMAN, R. L ; CARLINI, R. D ; COCHRAN, D. R. F ; FRANK, J. S ; PIASETZKY, E ; SANDBERG, V. D ; KRAKAUER, D. A ; TALAGA, R. L ; DOE, P. J ; HAUSAMMANN, R ; LEE, W. P ; LU, X. Q ; MHALER, H. J ; POTTER, M. E ; WANG, K. C ; BOWLES, T. J</creator><creatorcontrib>ALLEN, R. C ; CHEN, H. H ; BURMAN, R. L ; CARLINI, R. D ; COCHRAN, D. R. F ; FRANK, J. S ; PIASETZKY, E ; SANDBERG, V. D ; KRAKAUER, D. A ; TALAGA, R. L ; DOE, P. J ; HAUSAMMANN, R ; LEE, W. P ; LU, X. Q ; MHALER, H. J ; POTTER, M. E ; WANG, K. C ; BOWLES, T. J</creatorcontrib><description>Neutrino-electron elastic scattering was observed with a 15-ton fine-grained tracking calorimeter exposed to electron neutrinos from muon decay at rest. The measured [nu][sub [ital e]e][sup [minus]][r arrow][nu][sub [ital e]e][sup [minus]] elastic scattering rate of 236[plus minus]35 events yields the total elastic scattering cross section 10.0[plus minus]1.5(stat)[plus minus]0.9(syst)[times]10[sup [minus]45] cm[sup 2][times][[ital E][sub [nu]] (MeV)], and a model-independent measurement of the strength of the destructive interference between the charged and neutral currents, [ital I]=[minus]1.07[plus minus]0.21, that agrees well with the standard model (SM) prediction [ital I]=[minus]1.08. The agreement between the measured electroweak parameters and SM expectations is used to place limits on neutrino properties, such as neutrino flavor-changing neutral currents and neutrino electromagnetic moments. Limits are placed on the masses of new bosons that interact with leptons: for a neutral tensor boson, [ital M][sub [ital T]][gt]105 GeV; for a neutral (pseudo)scalar boson, [ital M][sub [ital P],][ital S][gt]47 GeV; for a charged Higgs boson, [ital M][sub [chi]][sup +][gt]87 GeV; and for a purely left-handed charged (neutral) vector boson, [ital M][sub [ital x]][gt]239 (119) GeV.</description><identifier>ISSN: 0556-2821</identifier><identifier>EISSN: 1089-4918</identifier><identifier>DOI: 10.1103/PhysRevD.47.11</identifier><identifier>PMID: 10015375</identifier><identifier>CODEN: PRVDAQ</identifier><language>eng</language><publisher>Ridge, NY: American Physical Society</publisher><subject>ACCELERATORS ; ALGEBRAIC CURRENTS ; BOSONS ; CALORIMETERS ; CHARGED CURRENTS ; COMPOSITE MODELS ; CROSS SECTIONS ; CURRENTS ; DECAY ; DIAGRAMS ; ELASTIC SCATTERING ; ELEMENTARY PARTICLES ; Exact sciences and technology ; FERMIONS ; FEYNMAN DIAGRAM ; FLAVOR MODEL ; HIGGS BOSONS ; INTERACTIONS ; INTERMEDIATE BOSONS ; INTERMEDIATE VECTOR BOSONS ; LAMPF LINAC ; LEPTON-LEPTON INTERACTIONS ; LEPTONS ; LINEAR ACCELERATORS ; MATHEMATICAL MODELS ; MEASURING INSTRUMENTS ; MESON FACTORIES ; MUONS ; NEUTRAL CURRENTS ; NEUTRINO-ELECTRON INTERACTIONS ; PARTICLE DECAY ; PARTICLE INTERACTIONS ; PARTICLE MODELS ; Physics ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; POSTULATED PARTICLES ; QUARK MODEL ; SCATTERING ; SPACE-TIME ; Specific reactions and phenomenology ; STANDARD MODEL ; The physics of elementary particles and fields ; TOTAL CROSS SECTIONS ; UNIFIED GAUGE MODELS 662310 -- Weak & Electromagnetic Interactions of Leptons-- (1992-) ; W MINUS BOSONS ; W PLUS BOSONS ; Weak and electromagnetic interactions of leptons ; Z NEUTRAL BOSONS</subject><ispartof>Physical review. D, Particles and fields, 1993, Vol.47 (1), p.11-28</ispartof><rights>1993 INIST-CNRS</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c349t-258a0833efd7be0b29a9900fb5cc65f7fc75d15e246188a3e33782ef7c6ce2fe3</citedby><cites>FETCH-LOGICAL-c349t-258a0833efd7be0b29a9900fb5cc65f7fc75d15e246188a3e33782ef7c6ce2fe3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,2862,2863,4009,27902,27903,27904</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=4492792$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/10015375$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/6786647$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>ALLEN, R. C</creatorcontrib><creatorcontrib>CHEN, H. H</creatorcontrib><creatorcontrib>BURMAN, R. L</creatorcontrib><creatorcontrib>CARLINI, R. D</creatorcontrib><creatorcontrib>COCHRAN, D. R. F</creatorcontrib><creatorcontrib>FRANK, J. S</creatorcontrib><creatorcontrib>PIASETZKY, E</creatorcontrib><creatorcontrib>SANDBERG, V. D</creatorcontrib><creatorcontrib>KRAKAUER, D. A</creatorcontrib><creatorcontrib>TALAGA, R. L</creatorcontrib><creatorcontrib>DOE, P. J</creatorcontrib><creatorcontrib>HAUSAMMANN, R</creatorcontrib><creatorcontrib>LEE, W. P</creatorcontrib><creatorcontrib>LU, X. Q</creatorcontrib><creatorcontrib>MHALER, H. J</creatorcontrib><creatorcontrib>POTTER, M. E</creatorcontrib><creatorcontrib>WANG, K. C</creatorcontrib><creatorcontrib>BOWLES, T. J</creatorcontrib><title>Study of electron-neutrino-electron elastic scattering at LAMPF</title><title>Physical review. D, Particles and fields</title><addtitle>Phys Rev D Part Fields</addtitle><description>Neutrino-electron elastic scattering was observed with a 15-ton fine-grained tracking calorimeter exposed to electron neutrinos from muon decay at rest. The measured [nu][sub [ital e]e][sup [minus]][r arrow][nu][sub [ital e]e][sup [minus]] elastic scattering rate of 236[plus minus]35 events yields the total elastic scattering cross section 10.0[plus minus]1.5(stat)[plus minus]0.9(syst)[times]10[sup [minus]45] cm[sup 2][times][[ital E][sub [nu]] (MeV)], and a model-independent measurement of the strength of the destructive interference between the charged and neutral currents, [ital I]=[minus]1.07[plus minus]0.21, that agrees well with the standard model (SM) prediction [ital I]=[minus]1.08. The agreement between the measured electroweak parameters and SM expectations is used to place limits on neutrino properties, such as neutrino flavor-changing neutral currents and neutrino electromagnetic moments. Limits are placed on the masses of new bosons that interact with leptons: for a neutral tensor boson, [ital M][sub [ital T]][gt]105 GeV; for a neutral (pseudo)scalar boson, [ital M][sub [ital P],][ital S][gt]47 GeV; for a charged Higgs boson, [ital M][sub [chi]][sup +][gt]87 GeV; and for a purely left-handed charged (neutral) vector boson, [ital M][sub [ital x]][gt]239 (119) GeV.</description><subject>ACCELERATORS</subject><subject>ALGEBRAIC CURRENTS</subject><subject>BOSONS</subject><subject>CALORIMETERS</subject><subject>CHARGED CURRENTS</subject><subject>COMPOSITE MODELS</subject><subject>CROSS SECTIONS</subject><subject>CURRENTS</subject><subject>DECAY</subject><subject>DIAGRAMS</subject><subject>ELASTIC SCATTERING</subject><subject>ELEMENTARY PARTICLES</subject><subject>Exact sciences and technology</subject><subject>FERMIONS</subject><subject>FEYNMAN DIAGRAM</subject><subject>FLAVOR MODEL</subject><subject>HIGGS BOSONS</subject><subject>INTERACTIONS</subject><subject>INTERMEDIATE BOSONS</subject><subject>INTERMEDIATE VECTOR BOSONS</subject><subject>LAMPF LINAC</subject><subject>LEPTON-LEPTON INTERACTIONS</subject><subject>LEPTONS</subject><subject>LINEAR ACCELERATORS</subject><subject>MATHEMATICAL MODELS</subject><subject>MEASURING INSTRUMENTS</subject><subject>MESON FACTORIES</subject><subject>MUONS</subject><subject>NEUTRAL CURRENTS</subject><subject>NEUTRINO-ELECTRON INTERACTIONS</subject><subject>PARTICLE DECAY</subject><subject>PARTICLE INTERACTIONS</subject><subject>PARTICLE MODELS</subject><subject>Physics</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>POSTULATED PARTICLES</subject><subject>QUARK MODEL</subject><subject>SCATTERING</subject><subject>SPACE-TIME</subject><subject>Specific reactions and phenomenology</subject><subject>STANDARD MODEL</subject><subject>The physics of elementary particles and fields</subject><subject>TOTAL CROSS SECTIONS</subject><subject>UNIFIED GAUGE MODELS 662310 -- Weak & Electromagnetic Interactions of Leptons-- (1992-)</subject><subject>W MINUS BOSONS</subject><subject>W PLUS BOSONS</subject><subject>Weak and electromagnetic interactions of leptons</subject><subject>Z NEUTRAL BOSONS</subject><issn>0556-2821</issn><issn>1089-4918</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNpNkEtLAzEUhYMotla3LmUQF26m5jGZJCsp1apQsfhYh0x6Y0emMzrJCP33RqYV7-bCOd99cBA6JXhMCGZXi9XGP8P3zTgTUdhDQ4KlSjNF5D4aYs7zlEpKBujI-w8ci-bsEA0IxoQzwYfo-iV0y03SuAQqsKFt6rSGLrRl3aQ7JVrGh9Im3poQIHrviQnJfPK4mB2jA2cqDyfbPkJvs9vX6X06f7p7mE7mqWWZCinl0mDJGLilKAAXVBmlMHYFtzbnTjgr-JJwoFlOpDQMGBOSghM2t0AdsBE67_c28RPtbRnArmxT1_FFnQuZ55mI0GUPfbbNVwc-6HXpLVSVqaHpvCaSK8qUlCSi4x61beN9C05_tuXatBtNsP5NVu-S1ZmIQhw42-7uijUs_-F9lBG42AIm5lS51tS29H9clikq4vUfoM6BeA</recordid><startdate>1993</startdate><enddate>1993</enddate><creator>ALLEN, R. C</creator><creator>CHEN, H. H</creator><creator>BURMAN, R. L</creator><creator>CARLINI, R. D</creator><creator>COCHRAN, D. R. F</creator><creator>FRANK, J. S</creator><creator>PIASETZKY, E</creator><creator>SANDBERG, V. D</creator><creator>KRAKAUER, D. A</creator><creator>TALAGA, R. L</creator><creator>DOE, P. J</creator><creator>HAUSAMMANN, R</creator><creator>LEE, W. P</creator><creator>LU, X. Q</creator><creator>MHALER, H. J</creator><creator>POTTER, M. E</creator><creator>WANG, K. C</creator><creator>BOWLES, T. J</creator><general>American Physical Society</general><scope>IQODW</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>1993</creationdate><title>Study of electron-neutrino-electron elastic scattering at LAMPF</title><author>ALLEN, R. C ; CHEN, H. H ; BURMAN, R. L ; CARLINI, R. D ; COCHRAN, D. R. F ; FRANK, J. S ; PIASETZKY, E ; SANDBERG, V. D ; KRAKAUER, D. A ; TALAGA, R. L ; DOE, P. J ; HAUSAMMANN, R ; LEE, W. P ; LU, X. Q ; MHALER, H. J ; POTTER, M. E ; WANG, K. C ; BOWLES, T. J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c349t-258a0833efd7be0b29a9900fb5cc65f7fc75d15e246188a3e33782ef7c6ce2fe3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>ACCELERATORS</topic><topic>ALGEBRAIC CURRENTS</topic><topic>BOSONS</topic><topic>CALORIMETERS</topic><topic>CHARGED CURRENTS</topic><topic>COMPOSITE MODELS</topic><topic>CROSS SECTIONS</topic><topic>CURRENTS</topic><topic>DECAY</topic><topic>DIAGRAMS</topic><topic>ELASTIC SCATTERING</topic><topic>ELEMENTARY PARTICLES</topic><topic>Exact sciences and technology</topic><topic>FERMIONS</topic><topic>FEYNMAN DIAGRAM</topic><topic>FLAVOR MODEL</topic><topic>HIGGS BOSONS</topic><topic>INTERACTIONS</topic><topic>INTERMEDIATE BOSONS</topic><topic>INTERMEDIATE VECTOR BOSONS</topic><topic>LAMPF LINAC</topic><topic>LEPTON-LEPTON INTERACTIONS</topic><topic>LEPTONS</topic><topic>LINEAR ACCELERATORS</topic><topic>MATHEMATICAL MODELS</topic><topic>MEASURING INSTRUMENTS</topic><topic>MESON FACTORIES</topic><topic>MUONS</topic><topic>NEUTRAL CURRENTS</topic><topic>NEUTRINO-ELECTRON INTERACTIONS</topic><topic>PARTICLE DECAY</topic><topic>PARTICLE INTERACTIONS</topic><topic>PARTICLE MODELS</topic><topic>Physics</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>POSTULATED PARTICLES</topic><topic>QUARK MODEL</topic><topic>SCATTERING</topic><topic>SPACE-TIME</topic><topic>Specific reactions and phenomenology</topic><topic>STANDARD MODEL</topic><topic>The physics of elementary particles and fields</topic><topic>TOTAL CROSS SECTIONS</topic><topic>UNIFIED GAUGE MODELS 662310 -- Weak & Electromagnetic Interactions of Leptons-- (1992-)</topic><topic>W MINUS BOSONS</topic><topic>W PLUS BOSONS</topic><topic>Weak and electromagnetic interactions of leptons</topic><topic>Z NEUTRAL BOSONS</topic><toplevel>online_resources</toplevel><creatorcontrib>ALLEN, R. 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D, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>ALLEN, R. C</au><au>CHEN, H. H</au><au>BURMAN, R. L</au><au>CARLINI, R. D</au><au>COCHRAN, D. R. F</au><au>FRANK, J. S</au><au>PIASETZKY, E</au><au>SANDBERG, V. D</au><au>KRAKAUER, D. A</au><au>TALAGA, R. L</au><au>DOE, P. J</au><au>HAUSAMMANN, R</au><au>LEE, W. P</au><au>LU, X. Q</au><au>MHALER, H. J</au><au>POTTER, M. E</au><au>WANG, K. C</au><au>BOWLES, T. J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Study of electron-neutrino-electron elastic scattering at LAMPF</atitle><jtitle>Physical review. D, Particles and fields</jtitle><addtitle>Phys Rev D Part Fields</addtitle><date>1993</date><risdate>1993</risdate><volume>47</volume><issue>1</issue><spage>11</spage><epage>28</epage><pages>11-28</pages><issn>0556-2821</issn><eissn>1089-4918</eissn><coden>PRVDAQ</coden><abstract>Neutrino-electron elastic scattering was observed with a 15-ton fine-grained tracking calorimeter exposed to electron neutrinos from muon decay at rest. The measured [nu][sub [ital e]e][sup [minus]][r arrow][nu][sub [ital e]e][sup [minus]] elastic scattering rate of 236[plus minus]35 events yields the total elastic scattering cross section 10.0[plus minus]1.5(stat)[plus minus]0.9(syst)[times]10[sup [minus]45] cm[sup 2][times][[ital E][sub [nu]] (MeV)], and a model-independent measurement of the strength of the destructive interference between the charged and neutral currents, [ital I]=[minus]1.07[plus minus]0.21, that agrees well with the standard model (SM) prediction [ital I]=[minus]1.08. The agreement between the measured electroweak parameters and SM expectations is used to place limits on neutrino properties, such as neutrino flavor-changing neutral currents and neutrino electromagnetic moments. Limits are placed on the masses of new bosons that interact with leptons: for a neutral tensor boson, [ital M][sub [ital T]][gt]105 GeV; for a neutral (pseudo)scalar boson, [ital M][sub [ital P],][ital S][gt]47 GeV; for a charged Higgs boson, [ital M][sub [chi]][sup +][gt]87 GeV; and for a purely left-handed charged (neutral) vector boson, [ital M][sub [ital x]][gt]239 (119) GeV.</abstract><cop>Ridge, NY</cop><pub>American Physical Society</pub><pmid>10015375</pmid><doi>10.1103/PhysRevD.47.11</doi><tpages>18</tpages></addata></record> |
| fulltext | fulltext |
| identifier | ISSN: 0556-2821 |
| ispartof | Physical review. D, Particles and fields, 1993, Vol.47 (1), p.11-28 |
| issn | 0556-2821 1089-4918 |
| language | eng |
| recordid | cdi_osti_scitechconnect_6786647 |
| source | American Physical Society Journals |
| subjects | ACCELERATORS ALGEBRAIC CURRENTS BOSONS CALORIMETERS CHARGED CURRENTS COMPOSITE MODELS CROSS SECTIONS CURRENTS DECAY DIAGRAMS ELASTIC SCATTERING ELEMENTARY PARTICLES Exact sciences and technology FERMIONS FEYNMAN DIAGRAM FLAVOR MODEL HIGGS BOSONS INTERACTIONS INTERMEDIATE BOSONS INTERMEDIATE VECTOR BOSONS LAMPF LINAC LEPTON-LEPTON INTERACTIONS LEPTONS LINEAR ACCELERATORS MATHEMATICAL MODELS MEASURING INSTRUMENTS MESON FACTORIES MUONS NEUTRAL CURRENTS NEUTRINO-ELECTRON INTERACTIONS PARTICLE DECAY PARTICLE INTERACTIONS PARTICLE MODELS Physics PHYSICS OF ELEMENTARY PARTICLES AND FIELDS POSTULATED PARTICLES QUARK MODEL SCATTERING SPACE-TIME Specific reactions and phenomenology STANDARD MODEL The physics of elementary particles and fields TOTAL CROSS SECTIONS UNIFIED GAUGE MODELS 662310 -- Weak & Electromagnetic Interactions of Leptons-- (1992-) W MINUS BOSONS W PLUS BOSONS Weak and electromagnetic interactions of leptons Z NEUTRAL BOSONS |
| title | Study of electron-neutrino-electron elastic scattering at LAMPF |
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