Dimuon production by neutrinos in the Fermilab 15-ft bubble chamber at the Tevatron
The Fermilab 15-ft bubble chamber has been exposed to a quadrupole triplet neutrino beam produced at the Tevatron. The ratio of {nu} to {bar {nu}} in the beam is approximately 2.5. The mean event energy for {nu}-induced charged-current events is 150 GeV, and for {bar {nu}}-induced charged-current ev...
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| Veröffentlicht in: | Physical review. D, Particles and fields Particles and fields, 1990-04, Vol.41 (7), p.2057-2073 |
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| container_title | Physical review. D, Particles and fields |
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| creator | Jain, V, V Harris, FA Aderholz, M Aggarwal, MM Akbari, H Allport, PP Baba, PV Badyal, SK Barth, M Baton, JP Bingham, HH Brucker, EB Burnstein, RA Campbell, JR Cence, RJ Chatterjee, TK Clayton, EF Corrigan, G Coutures, C Deprospo, D Devanand De Wolf E Faulkner, PJ Fretter, WB Gupta, VK Guy, J Hanlon, J Harigel, GG Jabiol, MA Jacques, P Jones, GT Jones, MD Kafka, T Kalelkar, M Kasper, P Kaul, GL Kaur, M Kohli, JM Koller, EL Krawiec, RJ Lauko, M Lys, J Marage, P Milburn, RH Miller, DB Mittra, IS Mobayyen, MM Moreels, J Morrison, DR Myatt, G Nailor, P Naon, R Napier, A Neveu, M Passmore, D Peters, MW Peterson, VZ Plano, R Rao, NK Rubin, HA Sacton, J Saitta, B Schmid, P Schmitz, N |
| description | The Fermilab 15-ft bubble chamber has been exposed to a quadrupole triplet neutrino beam produced at the Tevatron. The ratio of {nu} to {bar {nu}} in the beam is approximately 2.5. The mean event energy for {nu}-induced charged-current events is 150 GeV, and for {bar {nu}}-induced charged-current events it is 110 GeV. A total of 64 dimuon candidates (1 {mu}{sup +}{mu}{sup +}, 52 {mu}{sup {minus}}{mu}{sup +} and {mu}{sup +}{mu}{sup {minus}}, and 11 {mu}{sup {minus}}{mu}{sup {minus}}) is observed in the data sample of approximately 13 300 charged-current events. The number and properties of the {mu}{sup {minus}}{mu}{sup {minus}} and {mu}{sup +}{mu}{sup +} candidates are consistent with their being produced by background processes, the important sources being {pi} and {ital K} decay and punchthrough. The 90%-C.L. upper limit for {mu}{sup {minus}}{mu}{sup {minus}}/{mu}{sup {minus}} for muon momenta above 4 GeV/{ital c} is 1.2{times}10{sup {minus}3}, and for momenta above 9 GeV/{ital c} this limit is 1.1{times}10{sup {minus}3}. The opposite-sign-dimuon--to--single-muon ratio is (0.62{plus minus}0.13)% for muon momenta above 4 GeV/{ital c}. There are eight neutral strange particles in the opposite-sign sample, leading to a rate per dimuon event of 0.65{plus minus}0.29. The opposite-sign-dimuon sample is consistent with the hypothesis of charm production and decay. |
| doi_str_mv | 10.1103/PhysRevD.41.2057 |
| format | Article |
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The ratio of {nu} to {bar {nu}} in the beam is approximately 2.5. The mean event energy for {nu}-induced charged-current events is 150 GeV, and for {bar {nu}}-induced charged-current events it is 110 GeV. A total of 64 dimuon candidates (1 {mu}{sup +}{mu}{sup +}, 52 {mu}{sup {minus}}{mu}{sup +} and {mu}{sup +}{mu}{sup {minus}}, and 11 {mu}{sup {minus}}{mu}{sup {minus}}) is observed in the data sample of approximately 13 300 charged-current events. The number and properties of the {mu}{sup {minus}}{mu}{sup {minus}} and {mu}{sup +}{mu}{sup +} candidates are consistent with their being produced by background processes, the important sources being {pi} and {ital K} decay and punchthrough. The 90%-C.L. upper limit for {mu}{sup {minus}}{mu}{sup {minus}}/{mu}{sup {minus}} for muon momenta above 4 GeV/{ital c} is 1.2{times}10{sup {minus}3}, and for momenta above 9 GeV/{ital c} this limit is 1.1{times}10{sup {minus}3}. The opposite-sign-dimuon--to--single-muon ratio is (0.62{plus minus}0.13)% for muon momenta above 4 GeV/{ital c}. There are eight neutral strange particles in the opposite-sign sample, leading to a rate per dimuon event of 0.65{plus minus}0.29. The opposite-sign-dimuon sample is consistent with the hypothesis of charm production and decay.</description><identifier>ISSN: 0556-2821</identifier><identifier>EISSN: 1089-4918</identifier><identifier>DOI: 10.1103/PhysRevD.41.2057</identifier><identifier>PMID: 10012583</identifier><language>eng</language><publisher>United States</publisher><subject>ACCELERATORS ; ALKALINE EARTH METAL COMPOUNDS ; ANTINEUTRINO-NUCLEON INTERACTIONS ; BERYLLIUM COMPOUNDS ; BERYLLIUM OXIDES ; BUBBLE CHAMBERS ; CHALCOGENIDES ; CHARGED-CURRENT INTERACTIONS ; CHARM PARTICLES ; CYCLIC ACCELERATORS ; ELEMENTARY PARTICLES ; ENERGY RANGE ; ENERGY SPECTRA ; FERMILAB TEVATRON ; GAS TRACK DETECTORS ; GEV RANGE ; GEV RANGE 100-1000 ; INTERACTIONS ; LEPTON-BARYON INTERACTIONS ; LEPTON-HADRON INTERACTIONS ; LEPTON-NUCLEON INTERACTIONS ; MATHEMATICAL MODELS ; MEASURING INSTRUMENTS ; MONTE CARLO METHOD ; MUON PAIRS ; NEUTRINO-NUCLEON INTERACTIONS ; OXIDES ; OXYGEN COMPOUNDS ; PAIR PRODUCTION ; PARTICLE INTERACTIONS ; PARTICLE MODELS ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; RADIATION DETECTORS ; SPECTRA ; STANDARD MODEL ; STRANGE PARTICLES ; SYNCHROTRONS ; UNIFIED GAUGE MODELS 645102 -- High Energy Physics-- Particle Interactions & Properties-Experimental-- Weak Interactions & Properties</subject><ispartof>Physical review. D, Particles and fields, 1990-04, Vol.41 (7), p.2057-2073</ispartof><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c401t-7545d4a1e7677669517816e8ead32143a63ffea9a6b329b1a8bad1e9e0455d3e3</citedby><cites>FETCH-LOGICAL-c401t-7545d4a1e7677669517816e8ead32143a63ffea9a6b329b1a8bad1e9e0455d3e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,2876,2877,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/10012583$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/6829226$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Jain, V, V</creatorcontrib><creatorcontrib>Harris, FA</creatorcontrib><creatorcontrib>Aderholz, M</creatorcontrib><creatorcontrib>Aggarwal, MM</creatorcontrib><creatorcontrib>Akbari, H</creatorcontrib><creatorcontrib>Allport, PP</creatorcontrib><creatorcontrib>Baba, PV</creatorcontrib><creatorcontrib>Badyal, SK</creatorcontrib><creatorcontrib>Barth, M</creatorcontrib><creatorcontrib>Baton, JP</creatorcontrib><creatorcontrib>Bingham, HH</creatorcontrib><creatorcontrib>Brucker, EB</creatorcontrib><creatorcontrib>Burnstein, RA</creatorcontrib><creatorcontrib>Campbell, JR</creatorcontrib><creatorcontrib>Cence, RJ</creatorcontrib><creatorcontrib>Chatterjee, TK</creatorcontrib><creatorcontrib>Clayton, EF</creatorcontrib><creatorcontrib>Corrigan, G</creatorcontrib><creatorcontrib>Coutures, C</creatorcontrib><creatorcontrib>Deprospo, D</creatorcontrib><creatorcontrib>Devanand</creatorcontrib><creatorcontrib>De Wolf E</creatorcontrib><creatorcontrib>Faulkner, PJ</creatorcontrib><creatorcontrib>Fretter, WB</creatorcontrib><creatorcontrib>Gupta, VK</creatorcontrib><creatorcontrib>Guy, J</creatorcontrib><creatorcontrib>Hanlon, J</creatorcontrib><creatorcontrib>Harigel, GG</creatorcontrib><creatorcontrib>Jabiol, MA</creatorcontrib><creatorcontrib>Jacques, P</creatorcontrib><creatorcontrib>Jones, GT</creatorcontrib><creatorcontrib>Jones, MD</creatorcontrib><creatorcontrib>Kafka, T</creatorcontrib><creatorcontrib>Kalelkar, M</creatorcontrib><creatorcontrib>Kasper, P</creatorcontrib><creatorcontrib>Kaul, GL</creatorcontrib><creatorcontrib>Kaur, M</creatorcontrib><creatorcontrib>Kohli, JM</creatorcontrib><creatorcontrib>Koller, EL</creatorcontrib><creatorcontrib>Krawiec, RJ</creatorcontrib><creatorcontrib>Lauko, M</creatorcontrib><creatorcontrib>Lys, J</creatorcontrib><creatorcontrib>Marage, P</creatorcontrib><creatorcontrib>Milburn, RH</creatorcontrib><creatorcontrib>Miller, DB</creatorcontrib><creatorcontrib>Mittra, IS</creatorcontrib><creatorcontrib>Mobayyen, MM</creatorcontrib><creatorcontrib>Moreels, J</creatorcontrib><creatorcontrib>Morrison, DR</creatorcontrib><creatorcontrib>Myatt, G</creatorcontrib><creatorcontrib>Nailor, P</creatorcontrib><creatorcontrib>Naon, R</creatorcontrib><creatorcontrib>Napier, A</creatorcontrib><creatorcontrib>Neveu, M</creatorcontrib><creatorcontrib>Passmore, D</creatorcontrib><creatorcontrib>Peters, MW</creatorcontrib><creatorcontrib>Peterson, VZ</creatorcontrib><creatorcontrib>Plano, R</creatorcontrib><creatorcontrib>Rao, NK</creatorcontrib><creatorcontrib>Rubin, HA</creatorcontrib><creatorcontrib>Sacton, J</creatorcontrib><creatorcontrib>Saitta, B</creatorcontrib><creatorcontrib>Schmid, P</creatorcontrib><creatorcontrib>Schmitz, N</creatorcontrib><title>Dimuon production by neutrinos in the Fermilab 15-ft bubble chamber at the Tevatron</title><title>Physical review. D, Particles and fields</title><addtitle>Phys Rev D Part Fields</addtitle><description>The Fermilab 15-ft bubble chamber has been exposed to a quadrupole triplet neutrino beam produced at the Tevatron. The ratio of {nu} to {bar {nu}} in the beam is approximately 2.5. The mean event energy for {nu}-induced charged-current events is 150 GeV, and for {bar {nu}}-induced charged-current events it is 110 GeV. A total of 64 dimuon candidates (1 {mu}{sup +}{mu}{sup +}, 52 {mu}{sup {minus}}{mu}{sup +} and {mu}{sup +}{mu}{sup {minus}}, and 11 {mu}{sup {minus}}{mu}{sup {minus}}) is observed in the data sample of approximately 13 300 charged-current events. The number and properties of the {mu}{sup {minus}}{mu}{sup {minus}} and {mu}{sup +}{mu}{sup +} candidates are consistent with their being produced by background processes, the important sources being {pi} and {ital K} decay and punchthrough. The 90%-C.L. upper limit for {mu}{sup {minus}}{mu}{sup {minus}}/{mu}{sup {minus}} for muon momenta above 4 GeV/{ital c} is 1.2{times}10{sup {minus}3}, and for momenta above 9 GeV/{ital c} this limit is 1.1{times}10{sup {minus}3}. The opposite-sign-dimuon--to--single-muon ratio is (0.62{plus minus}0.13)% for muon momenta above 4 GeV/{ital c}. There are eight neutral strange particles in the opposite-sign sample, leading to a rate per dimuon event of 0.65{plus minus}0.29. The opposite-sign-dimuon sample is consistent with the hypothesis of charm production and decay.</description><subject>ACCELERATORS</subject><subject>ALKALINE EARTH METAL COMPOUNDS</subject><subject>ANTINEUTRINO-NUCLEON INTERACTIONS</subject><subject>BERYLLIUM COMPOUNDS</subject><subject>BERYLLIUM OXIDES</subject><subject>BUBBLE CHAMBERS</subject><subject>CHALCOGENIDES</subject><subject>CHARGED-CURRENT INTERACTIONS</subject><subject>CHARM PARTICLES</subject><subject>CYCLIC ACCELERATORS</subject><subject>ELEMENTARY PARTICLES</subject><subject>ENERGY RANGE</subject><subject>ENERGY SPECTRA</subject><subject>FERMILAB TEVATRON</subject><subject>GAS TRACK DETECTORS</subject><subject>GEV RANGE</subject><subject>GEV RANGE 100-1000</subject><subject>INTERACTIONS</subject><subject>LEPTON-BARYON INTERACTIONS</subject><subject>LEPTON-HADRON INTERACTIONS</subject><subject>LEPTON-NUCLEON INTERACTIONS</subject><subject>MATHEMATICAL MODELS</subject><subject>MEASURING INSTRUMENTS</subject><subject>MONTE CARLO METHOD</subject><subject>MUON PAIRS</subject><subject>NEUTRINO-NUCLEON INTERACTIONS</subject><subject>OXIDES</subject><subject>OXYGEN COMPOUNDS</subject><subject>PAIR PRODUCTION</subject><subject>PARTICLE INTERACTIONS</subject><subject>PARTICLE MODELS</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>RADIATION DETECTORS</subject><subject>SPECTRA</subject><subject>STANDARD MODEL</subject><subject>STRANGE PARTICLES</subject><subject>SYNCHROTRONS</subject><subject>UNIFIED GAUGE MODELS 645102 -- High Energy Physics-- Particle Interactions & Properties-Experimental-- Weak Interactions & 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ELEMENTARY PARTICLES AND FIELDS</topic><topic>RADIATION DETECTORS</topic><topic>SPECTRA</topic><topic>STANDARD MODEL</topic><topic>STRANGE PARTICLES</topic><topic>SYNCHROTRONS</topic><topic>UNIFIED GAUGE MODELS 645102 -- High Energy Physics-- Particle Interactions & Properties-Experimental-- Weak Interactions & Properties</topic><toplevel>online_resources</toplevel><creatorcontrib>Jain, V, V</creatorcontrib><creatorcontrib>Harris, FA</creatorcontrib><creatorcontrib>Aderholz, M</creatorcontrib><creatorcontrib>Aggarwal, MM</creatorcontrib><creatorcontrib>Akbari, H</creatorcontrib><creatorcontrib>Allport, PP</creatorcontrib><creatorcontrib>Baba, PV</creatorcontrib><creatorcontrib>Badyal, SK</creatorcontrib><creatorcontrib>Barth, M</creatorcontrib><creatorcontrib>Baton, JP</creatorcontrib><creatorcontrib>Bingham, HH</creatorcontrib><creatorcontrib>Brucker, EB</creatorcontrib><creatorcontrib>Burnstein, RA</creatorcontrib><creatorcontrib>Campbell, JR</creatorcontrib><creatorcontrib>Cence, RJ</creatorcontrib><creatorcontrib>Chatterjee, TK</creatorcontrib><creatorcontrib>Clayton, EF</creatorcontrib><creatorcontrib>Corrigan, G</creatorcontrib><creatorcontrib>Coutures, C</creatorcontrib><creatorcontrib>Deprospo, D</creatorcontrib><creatorcontrib>Devanand</creatorcontrib><creatorcontrib>De Wolf E</creatorcontrib><creatorcontrib>Faulkner, PJ</creatorcontrib><creatorcontrib>Fretter, WB</creatorcontrib><creatorcontrib>Gupta, VK</creatorcontrib><creatorcontrib>Guy, J</creatorcontrib><creatorcontrib>Hanlon, J</creatorcontrib><creatorcontrib>Harigel, GG</creatorcontrib><creatorcontrib>Jabiol, MA</creatorcontrib><creatorcontrib>Jacques, P</creatorcontrib><creatorcontrib>Jones, GT</creatorcontrib><creatorcontrib>Jones, MD</creatorcontrib><creatorcontrib>Kafka, T</creatorcontrib><creatorcontrib>Kalelkar, M</creatorcontrib><creatorcontrib>Kasper, P</creatorcontrib><creatorcontrib>Kaul, GL</creatorcontrib><creatorcontrib>Kaur, M</creatorcontrib><creatorcontrib>Kohli, JM</creatorcontrib><creatorcontrib>Koller, EL</creatorcontrib><creatorcontrib>Krawiec, RJ</creatorcontrib><creatorcontrib>Lauko, M</creatorcontrib><creatorcontrib>Lys, J</creatorcontrib><creatorcontrib>Marage, P</creatorcontrib><creatorcontrib>Milburn, RH</creatorcontrib><creatorcontrib>Miller, DB</creatorcontrib><creatorcontrib>Mittra, IS</creatorcontrib><creatorcontrib>Mobayyen, MM</creatorcontrib><creatorcontrib>Moreels, J</creatorcontrib><creatorcontrib>Morrison, DR</creatorcontrib><creatorcontrib>Myatt, G</creatorcontrib><creatorcontrib>Nailor, P</creatorcontrib><creatorcontrib>Naon, R</creatorcontrib><creatorcontrib>Napier, A</creatorcontrib><creatorcontrib>Neveu, M</creatorcontrib><creatorcontrib>Passmore, D</creatorcontrib><creatorcontrib>Peters, MW</creatorcontrib><creatorcontrib>Peterson, VZ</creatorcontrib><creatorcontrib>Plano, R</creatorcontrib><creatorcontrib>Rao, NK</creatorcontrib><creatorcontrib>Rubin, HA</creatorcontrib><creatorcontrib>Sacton, J</creatorcontrib><creatorcontrib>Saitta, B</creatorcontrib><creatorcontrib>Schmid, P</creatorcontrib><creatorcontrib>Schmitz, N</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Physical review. D, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Jain, V, V</au><au>Harris, FA</au><au>Aderholz, M</au><au>Aggarwal, MM</au><au>Akbari, H</au><au>Allport, PP</au><au>Baba, PV</au><au>Badyal, SK</au><au>Barth, M</au><au>Baton, JP</au><au>Bingham, HH</au><au>Brucker, EB</au><au>Burnstein, RA</au><au>Campbell, JR</au><au>Cence, RJ</au><au>Chatterjee, TK</au><au>Clayton, EF</au><au>Corrigan, G</au><au>Coutures, C</au><au>Deprospo, D</au><au>Devanand</au><au>De Wolf E</au><au>Faulkner, PJ</au><au>Fretter, WB</au><au>Gupta, VK</au><au>Guy, J</au><au>Hanlon, J</au><au>Harigel, GG</au><au>Jabiol, MA</au><au>Jacques, P</au><au>Jones, GT</au><au>Jones, MD</au><au>Kafka, T</au><au>Kalelkar, M</au><au>Kasper, P</au><au>Kaul, GL</au><au>Kaur, M</au><au>Kohli, JM</au><au>Koller, EL</au><au>Krawiec, RJ</au><au>Lauko, M</au><au>Lys, J</au><au>Marage, P</au><au>Milburn, RH</au><au>Miller, DB</au><au>Mittra, IS</au><au>Mobayyen, MM</au><au>Moreels, J</au><au>Morrison, DR</au><au>Myatt, G</au><au>Nailor, P</au><au>Naon, R</au><au>Napier, A</au><au>Neveu, M</au><au>Passmore, D</au><au>Peters, MW</au><au>Peterson, VZ</au><au>Plano, R</au><au>Rao, NK</au><au>Rubin, HA</au><au>Sacton, J</au><au>Saitta, B</au><au>Schmid, P</au><au>Schmitz, N</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dimuon production by neutrinos in the Fermilab 15-ft bubble chamber at the Tevatron</atitle><jtitle>Physical review. D, Particles and fields</jtitle><addtitle>Phys Rev D Part Fields</addtitle><date>1990-04-01</date><risdate>1990</risdate><volume>41</volume><issue>7</issue><spage>2057</spage><epage>2073</epage><pages>2057-2073</pages><issn>0556-2821</issn><eissn>1089-4918</eissn><abstract>The Fermilab 15-ft bubble chamber has been exposed to a quadrupole triplet neutrino beam produced at the Tevatron. The ratio of {nu} to {bar {nu}} in the beam is approximately 2.5. The mean event energy for {nu}-induced charged-current events is 150 GeV, and for {bar {nu}}-induced charged-current events it is 110 GeV. A total of 64 dimuon candidates (1 {mu}{sup +}{mu}{sup +}, 52 {mu}{sup {minus}}{mu}{sup +} and {mu}{sup +}{mu}{sup {minus}}, and 11 {mu}{sup {minus}}{mu}{sup {minus}}) is observed in the data sample of approximately 13 300 charged-current events. The number and properties of the {mu}{sup {minus}}{mu}{sup {minus}} and {mu}{sup +}{mu}{sup +} candidates are consistent with their being produced by background processes, the important sources being {pi} and {ital K} decay and punchthrough. The 90%-C.L. upper limit for {mu}{sup {minus}}{mu}{sup {minus}}/{mu}{sup {minus}} for muon momenta above 4 GeV/{ital c} is 1.2{times}10{sup {minus}3}, and for momenta above 9 GeV/{ital c} this limit is 1.1{times}10{sup {minus}3}. The opposite-sign-dimuon--to--single-muon ratio is (0.62{plus minus}0.13)% for muon momenta above 4 GeV/{ital c}. There are eight neutral strange particles in the opposite-sign sample, leading to a rate per dimuon event of 0.65{plus minus}0.29. The opposite-sign-dimuon sample is consistent with the hypothesis of charm production and decay.</abstract><cop>United States</cop><pmid>10012583</pmid><doi>10.1103/PhysRevD.41.2057</doi><tpages>17</tpages><oa>free_for_read</oa></addata></record> |
| fulltext | fulltext |
| identifier | ISSN: 0556-2821 |
| ispartof | Physical review. D, Particles and fields, 1990-04, Vol.41 (7), p.2057-2073 |
| issn | 0556-2821 1089-4918 |
| language | eng |
| recordid | cdi_osti_scitechconnect_6829226 |
| source | American Physical Society Journals |
| subjects | ACCELERATORS ALKALINE EARTH METAL COMPOUNDS ANTINEUTRINO-NUCLEON INTERACTIONS BERYLLIUM COMPOUNDS BERYLLIUM OXIDES BUBBLE CHAMBERS CHALCOGENIDES CHARGED-CURRENT INTERACTIONS CHARM PARTICLES CYCLIC ACCELERATORS ELEMENTARY PARTICLES ENERGY RANGE ENERGY SPECTRA FERMILAB TEVATRON GAS TRACK DETECTORS GEV RANGE GEV RANGE 100-1000 INTERACTIONS LEPTON-BARYON INTERACTIONS LEPTON-HADRON INTERACTIONS LEPTON-NUCLEON INTERACTIONS MATHEMATICAL MODELS MEASURING INSTRUMENTS MONTE CARLO METHOD MUON PAIRS NEUTRINO-NUCLEON INTERACTIONS OXIDES OXYGEN COMPOUNDS PAIR PRODUCTION PARTICLE INTERACTIONS PARTICLE MODELS PHYSICS OF ELEMENTARY PARTICLES AND FIELDS RADIATION DETECTORS SPECTRA STANDARD MODEL STRANGE PARTICLES SYNCHROTRONS UNIFIED GAUGE MODELS 645102 -- High Energy Physics-- Particle Interactions & Properties-Experimental-- Weak Interactions & Properties |
| title | Dimuon production by neutrinos in the Fermilab 15-ft bubble chamber at the Tevatron |
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