Coherent production of single pions and [rho] mesons in charged-current interactions of neutrinos and antineutrinos on neon nuclei at the Fermilab Tevatron
The coherent production of [pi] and [rho] mesons in [nu][sub [mu]]([bar [nu]][sub [mu]])--neon charged-current interactions has been studied using the Fermilab 15-foot bubble chamber filled with a heavy Ne-H[sub 2] mix and exposed to the Teva- tron quadrupole triplet (anti)neutrino beam. The [nu][su...
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creator | Willocq, S. Aderholz, M. Akbari, H. Allport, P.P. Badyal, S.K. Ballagh, H.C. Barth, M. Bingham, H.H. Brucker, E.B. Burnstein, R.A. Cence, R.J. Chatterjee, T.K. Clayton, E.F. Corrigan, G. De Prospo, D. Devanand De Wolf, E. Faulkner, P.J.W. Foeth, H. Fretter, W.B. Gupta, V.K. Hanlon, J. Harigel, G. Harris, F.A. Jacques, P. Jain, V. Jones, G.T. Jones, M.D. Kafka, T. Kalelkar, M. Kohli, J.M. Koller, E.L. Krawiec, R.J. Lauko, M. Lys, J.E. Marage, P. Milburn, R.H. Mittra, I.S. Mobayyen, M.M. Moreels, J. Morrison, D.R.O. Myatt, G. Nailor, P. Naon, R. Napier, A. Passmore, D. Peters, M.W. Peterson, V.Z. Plano, R. Rao, N.K. Rubin, H.A. Sacton, J. Sambyal, S.S. Schmitz, N. Schneps, J. Singh, J.B. Singh, S. Smart, W. Stamer, P. Varvell, K.E. Verluyten, L. Wachsmuth, H. Wainstein, S. Yost, G.P. |
description | The coherent production of [pi] and [rho] mesons in [nu][sub [mu]]([bar [nu]][sub [mu]])--neon charged-current interactions has been studied using the Fermilab 15-foot bubble chamber filled with a heavy Ne-H[sub 2] mix and exposed to the Teva- tron quadrupole triplet (anti)neutrino beam. The [nu][sub [mu]] ([bar [nu]][sub [mu]]) beam had an average energy of 80 GeV (70 GeV). From a sample corresponding to approximately 28 000 charged-current interactions, net signals of (53[plus minus]9) [mu][sup [plus minus]][pi][sup [minus plus]] coherent events and (19[plus minus]7) [mu][sup [plus minus]][pi][sup [minus plus]][pi][sup 0] coherent events are extracted. For [ital E][gt]10 GeV, the coherent pion production cross section is determined to be (3.2[plus minus]0.7)[times]10[sup [minus]38] cm[sup 2] per neon nucleus whereas the coherent [rho] production cross section is (2.1[plus minus]0.8)[times]10[sup [minus]38] cm[sup 2] per neon nucleus. These cross sections and the kinematical characteristics of the coherent events at [vert bar][ital t][vert bar][lt]0.1 GeV[sup 2] are found to be in general agreement with the predictions of a model based on the hadron dominance and, in the pion case, on the partially conserved axial-vector current hypothesis. Also discussed is the coherent production of systems consisting of three pions. |
doi_str_mv | 10.1103/PhysRevD.47.2661 |
format | Article |
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The [nu][sub [mu]] ([bar [nu]][sub [mu]]) beam had an average energy of 80 GeV (70 GeV). From a sample corresponding to approximately 28 000 charged-current interactions, net signals of (53[plus minus]9) [mu][sup [plus minus]][pi][sup [minus plus]] coherent events and (19[plus minus]7) [mu][sup [plus minus]][pi][sup [minus plus]][pi][sup 0] coherent events are extracted. For [ital E][gt]10 GeV, the coherent pion production cross section is determined to be (3.2[plus minus]0.7)[times]10[sup [minus]38] cm[sup 2] per neon nucleus whereas the coherent [rho] production cross section is (2.1[plus minus]0.8)[times]10[sup [minus]38] cm[sup 2] per neon nucleus. These cross sections and the kinematical characteristics of the coherent events at [vert bar][ital t][vert bar][lt]0.1 GeV[sup 2] are found to be in general agreement with the predictions of a model based on the hadron dominance and, in the pion case, on the partially conserved axial-vector current hypothesis. Also discussed is the coherent production of systems consisting of three pions.</description><identifier>ISSN: 0556-2821</identifier><identifier>EISSN: 1089-4918</identifier><identifier>DOI: 10.1103/PhysRevD.47.2661</identifier><language>eng</language><publisher>United States</publisher><subject>ANTINEUTRINO-NUCLEON INTERACTIONS ; BOSONS ; BUBBLE CHAMBERS ; CROSS SECTIONS ; DATA ; ELEMENTARY PARTICLES ; ELEMENTS ; EXPERIMENTAL DATA ; FLUIDS ; GAS TRACK DETECTORS ; GASES ; HADRONS ; HYDROGEN ; INFORMATION ; INTERACTIONS ; LEPTON-BARYON INTERACTIONS ; LEPTON-HADRON INTERACTIONS ; LEPTON-NUCLEON INTERACTIONS ; MEASURING INSTRUMENTS ; MESONS ; NEON ; NEUTRINO-NUCLEON INTERACTIONS ; NONMETALS ; NUMERICAL DATA ; PARTICLE INTERACTIONS ; PARTICLE KINEMATICS ; PARTICLE PRODUCTION ; PCAC THEORY ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; PIONS ; PSEUDOSCALAR MESONS ; RADIATION DETECTORS ; RARE GASES ; RHO-770 MESONS ; VECTOR MESONS 662320 -- Neutrino Interactions-- (1992-)</subject><ispartof>Physical review. 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D, Particles and fields</title><description>The coherent production of [pi] and [rho] mesons in [nu][sub [mu]]([bar [nu]][sub [mu]])--neon charged-current interactions has been studied using the Fermilab 15-foot bubble chamber filled with a heavy Ne-H[sub 2] mix and exposed to the Teva- tron quadrupole triplet (anti)neutrino beam. The [nu][sub [mu]] ([bar [nu]][sub [mu]]) beam had an average energy of 80 GeV (70 GeV). From a sample corresponding to approximately 28 000 charged-current interactions, net signals of (53[plus minus]9) [mu][sup [plus minus]][pi][sup [minus plus]] coherent events and (19[plus minus]7) [mu][sup [plus minus]][pi][sup [minus plus]][pi][sup 0] coherent events are extracted. For [ital E][gt]10 GeV, the coherent pion production cross section is determined to be (3.2[plus minus]0.7)[times]10[sup [minus]38] cm[sup 2] per neon nucleus whereas the coherent [rho] production cross section is (2.1[plus minus]0.8)[times]10[sup [minus]38] cm[sup 2] per neon nucleus. These cross sections and the kinematical characteristics of the coherent events at [vert bar][ital t][vert bar][lt]0.1 GeV[sup 2] are found to be in general agreement with the predictions of a model based on the hadron dominance and, in the pion case, on the partially conserved axial-vector current hypothesis. Also discussed is the coherent production of systems consisting of three pions.</description><subject>ANTINEUTRINO-NUCLEON INTERACTIONS</subject><subject>BOSONS</subject><subject>BUBBLE CHAMBERS</subject><subject>CROSS SECTIONS</subject><subject>DATA</subject><subject>ELEMENTARY PARTICLES</subject><subject>ELEMENTS</subject><subject>EXPERIMENTAL DATA</subject><subject>FLUIDS</subject><subject>GAS TRACK DETECTORS</subject><subject>GASES</subject><subject>HADRONS</subject><subject>HYDROGEN</subject><subject>INFORMATION</subject><subject>INTERACTIONS</subject><subject>LEPTON-BARYON INTERACTIONS</subject><subject>LEPTON-HADRON INTERACTIONS</subject><subject>LEPTON-NUCLEON INTERACTIONS</subject><subject>MEASURING INSTRUMENTS</subject><subject>MESONS</subject><subject>NEON</subject><subject>NEUTRINO-NUCLEON INTERACTIONS</subject><subject>NONMETALS</subject><subject>NUMERICAL DATA</subject><subject>PARTICLE INTERACTIONS</subject><subject>PARTICLE KINEMATICS</subject><subject>PARTICLE PRODUCTION</subject><subject>PCAC THEORY</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>PIONS</subject><subject>PSEUDOSCALAR MESONS</subject><subject>RADIATION DETECTORS</subject><subject>RARE GASES</subject><subject>RHO-770 MESONS</subject><subject>VECTOR MESONS 662320 -- Neutrino Interactions-- (1992-)</subject><issn>0556-2821</issn><issn>1089-4918</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNpFj0tLAzEUhYMoWKt7l8H91DwmmZmlVKtCQZHuREoedzqRaVKSTMHf4p91agXv4h7uge8cLkLXlMwoJfz2tftKb7C_n5XVjElJT9CEkropyobWp2hChJAFqxk9RxcpfZJxmOQT9D0PHUTwGe9isIPJLngcWpyc3_SAd-OZsPIWv8cufOAtpIPhPDadihuwhRniL-58hqh--XQI8DDk6Hw40spn9--MFR4OazA9OKwyzh3gBcSt65XGK9irHIO_RGet6hNc_ekUrRYPq_lTsXx5fJ7fLYvQiFwosEyWilotKiFtKRpquSS6AtlKZmo7vmoZaVqitTRcEy4oIa2x2lRW1IpP0c0xNqTs1sm4DKYzwXsweS2lEExw_gNft29H</recordid><startdate>19930401</startdate><enddate>19930401</enddate><creator>Willocq, 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G.P.</creator><scope>OTOTI</scope></search><sort><creationdate>19930401</creationdate><title>Coherent production of single pions and [rho] mesons in charged-current interactions of neutrinos and antineutrinos on neon nuclei at the Fermilab Tevatron</title><author>Willocq, S. ; Aderholz, M. ; Akbari, H. ; Allport, P.P. ; Badyal, S.K. ; Ballagh, H.C. ; Barth, M. ; Bingham, H.H. ; Brucker, E.B. ; Burnstein, R.A. ; Cence, R.J. ; Chatterjee, T.K. ; Clayton, E.F. ; Corrigan, G. ; De Prospo, D. ; Devanand ; De Wolf, E. ; Faulkner, P.J.W. ; Foeth, H. ; Fretter, W.B. ; Gupta, V.K. ; Hanlon, J. ; Harigel, G. ; Harris, F.A. ; Jacques, P. ; Jain, V. ; Jones, G.T. ; Jones, M.D. ; Kafka, T. ; Kalelkar, M. ; Kohli, J.M. ; Koller, E.L. ; Krawiec, R.J. ; Lauko, M. ; Lys, J.E. ; Marage, P. ; Milburn, R.H. ; Mittra, I.S. ; Mobayyen, M.M. ; Moreels, J. ; Morrison, D.R.O. ; Myatt, G. ; Nailor, P. ; Naon, R. ; Napier, A. ; Passmore, D. ; Peters, M.W. ; Peterson, V.Z. ; Plano, R. ; Rao, N.K. ; Rubin, H.A. ; Sacton, J. ; Sambyal, S.S. ; Schmitz, N. ; Schneps, J. ; Singh, J.B. ; Singh, S. ; Smart, W. ; Stamer, P. ; Varvell, K.E. ; Verluyten, L. ; Wachsmuth, H. ; Wainstein, S. ; Yost, G.P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o95t-aed264a1db5756d4591d360b7e6f62c8d000d209f0bb6c3b035100fcdbc7d58a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>ANTINEUTRINO-NUCLEON INTERACTIONS</topic><topic>BOSONS</topic><topic>BUBBLE CHAMBERS</topic><topic>CROSS SECTIONS</topic><topic>DATA</topic><topic>ELEMENTARY PARTICLES</topic><topic>ELEMENTS</topic><topic>EXPERIMENTAL DATA</topic><topic>FLUIDS</topic><topic>GAS TRACK DETECTORS</topic><topic>GASES</topic><topic>HADRONS</topic><topic>HYDROGEN</topic><topic>INFORMATION</topic><topic>INTERACTIONS</topic><topic>LEPTON-BARYON INTERACTIONS</topic><topic>LEPTON-HADRON INTERACTIONS</topic><topic>LEPTON-NUCLEON INTERACTIONS</topic><topic>MEASURING INSTRUMENTS</topic><topic>MESONS</topic><topic>NEON</topic><topic>NEUTRINO-NUCLEON INTERACTIONS</topic><topic>NONMETALS</topic><topic>NUMERICAL DATA</topic><topic>PARTICLE INTERACTIONS</topic><topic>PARTICLE KINEMATICS</topic><topic>PARTICLE PRODUCTION</topic><topic>PCAC THEORY</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>PIONS</topic><topic>PSEUDOSCALAR MESONS</topic><topic>RADIATION DETECTORS</topic><topic>RARE GASES</topic><topic>RHO-770 MESONS</topic><topic>VECTOR MESONS 662320 -- Neutrino Interactions-- (1992-)</topic><toplevel>online_resources</toplevel><creatorcontrib>Willocq, S.</creatorcontrib><creatorcontrib>Aderholz, M.</creatorcontrib><creatorcontrib>Akbari, H.</creatorcontrib><creatorcontrib>Allport, P.P.</creatorcontrib><creatorcontrib>Badyal, S.K.</creatorcontrib><creatorcontrib>Ballagh, H.C.</creatorcontrib><creatorcontrib>Barth, M.</creatorcontrib><creatorcontrib>Bingham, H.H.</creatorcontrib><creatorcontrib>Brucker, E.B.</creatorcontrib><creatorcontrib>Burnstein, R.A.</creatorcontrib><creatorcontrib>Cence, R.J.</creatorcontrib><creatorcontrib>Chatterjee, T.K.</creatorcontrib><creatorcontrib>Clayton, E.F.</creatorcontrib><creatorcontrib>Corrigan, G.</creatorcontrib><creatorcontrib>De Prospo, D.</creatorcontrib><creatorcontrib>Devanand</creatorcontrib><creatorcontrib>De Wolf, E.</creatorcontrib><creatorcontrib>Faulkner, P.J.W.</creatorcontrib><creatorcontrib>Foeth, H.</creatorcontrib><creatorcontrib>Fretter, W.B.</creatorcontrib><creatorcontrib>Gupta, V.K.</creatorcontrib><creatorcontrib>Hanlon, J.</creatorcontrib><creatorcontrib>Harigel, G.</creatorcontrib><creatorcontrib>Harris, F.A.</creatorcontrib><creatorcontrib>Jacques, P.</creatorcontrib><creatorcontrib>Jain, V.</creatorcontrib><creatorcontrib>Jones, G.T.</creatorcontrib><creatorcontrib>Jones, M.D.</creatorcontrib><creatorcontrib>Kafka, T.</creatorcontrib><creatorcontrib>Kalelkar, M.</creatorcontrib><creatorcontrib>Kohli, J.M.</creatorcontrib><creatorcontrib>Koller, E.L.</creatorcontrib><creatorcontrib>Krawiec, R.J.</creatorcontrib><creatorcontrib>Lauko, M.</creatorcontrib><creatorcontrib>Lys, J.E.</creatorcontrib><creatorcontrib>Marage, P.</creatorcontrib><creatorcontrib>Milburn, R.H.</creatorcontrib><creatorcontrib>Mittra, I.S.</creatorcontrib><creatorcontrib>Mobayyen, M.M.</creatorcontrib><creatorcontrib>Moreels, J.</creatorcontrib><creatorcontrib>Morrison, D.R.O.</creatorcontrib><creatorcontrib>Myatt, G.</creatorcontrib><creatorcontrib>Nailor, P.</creatorcontrib><creatorcontrib>Naon, R.</creatorcontrib><creatorcontrib>Napier, A.</creatorcontrib><creatorcontrib>Passmore, D.</creatorcontrib><creatorcontrib>Peters, M.W.</creatorcontrib><creatorcontrib>Peterson, V.Z.</creatorcontrib><creatorcontrib>Plano, R.</creatorcontrib><creatorcontrib>Rao, N.K.</creatorcontrib><creatorcontrib>Rubin, H.A.</creatorcontrib><creatorcontrib>Sacton, J.</creatorcontrib><creatorcontrib>Sambyal, S.S.</creatorcontrib><creatorcontrib>Schmitz, N.</creatorcontrib><creatorcontrib>Schneps, J.</creatorcontrib><creatorcontrib>Singh, J.B.</creatorcontrib><creatorcontrib>Singh, S.</creatorcontrib><creatorcontrib>Smart, W.</creatorcontrib><creatorcontrib>Stamer, P.</creatorcontrib><creatorcontrib>Varvell, K.E.</creatorcontrib><creatorcontrib>Verluyten, L.</creatorcontrib><creatorcontrib>Wachsmuth, H.</creatorcontrib><creatorcontrib>Wainstein, S.</creatorcontrib><creatorcontrib>Yost, G.P.</creatorcontrib><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>Willocq, S.</au><au>Aderholz, M.</au><au>Akbari, H.</au><au>Allport, P.P.</au><au>Badyal, S.K.</au><au>Ballagh, H.C.</au><au>Barth, M.</au><au>Bingham, H.H.</au><au>Brucker, E.B.</au><au>Burnstein, R.A.</au><au>Cence, R.J.</au><au>Chatterjee, T.K.</au><au>Clayton, E.F.</au><au>Corrigan, G.</au><au>De Prospo, D.</au><au>Devanand</au><au>De Wolf, E.</au><au>Faulkner, P.J.W.</au><au>Foeth, H.</au><au>Fretter, W.B.</au><au>Gupta, V.K.</au><au>Hanlon, J.</au><au>Harigel, G.</au><au>Harris, F.A.</au><au>Jacques, P.</au><au>Jain, V.</au><au>Jones, G.T.</au><au>Jones, M.D.</au><au>Kafka, T.</au><au>Kalelkar, M.</au><au>Kohli, J.M.</au><au>Koller, E.L.</au><au>Krawiec, R.J.</au><au>Lauko, M.</au><au>Lys, J.E.</au><au>Marage, P.</au><au>Milburn, R.H.</au><au>Mittra, I.S.</au><au>Mobayyen, M.M.</au><au>Moreels, J.</au><au>Morrison, D.R.O.</au><au>Myatt, G.</au><au>Nailor, P.</au><au>Naon, R.</au><au>Napier, A.</au><au>Passmore, D.</au><au>Peters, M.W.</au><au>Peterson, V.Z.</au><au>Plano, R.</au><au>Rao, N.K.</au><au>Rubin, H.A.</au><au>Sacton, J.</au><au>Sambyal, S.S.</au><au>Schmitz, N.</au><au>Schneps, J.</au><au>Singh, J.B.</au><au>Singh, S.</au><au>Smart, W.</au><au>Stamer, P.</au><au>Varvell, K.E.</au><au>Verluyten, L.</au><au>Wachsmuth, H.</au><au>Wainstein, S.</au><au>Yost, G.P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Coherent production of single pions and [rho] mesons in charged-current interactions of neutrinos and antineutrinos on neon nuclei at the Fermilab Tevatron</atitle><jtitle>Physical review. D, Particles and fields</jtitle><date>1993-04-01</date><risdate>1993</risdate><volume>47:7</volume><issn>0556-2821</issn><eissn>1089-4918</eissn><abstract>The coherent production of [pi] and [rho] mesons in [nu][sub [mu]]([bar [nu]][sub [mu]])--neon charged-current interactions has been studied using the Fermilab 15-foot bubble chamber filled with a heavy Ne-H[sub 2] mix and exposed to the Teva- tron quadrupole triplet (anti)neutrino beam. The [nu][sub [mu]] ([bar [nu]][sub [mu]]) beam had an average energy of 80 GeV (70 GeV). From a sample corresponding to approximately 28 000 charged-current interactions, net signals of (53[plus minus]9) [mu][sup [plus minus]][pi][sup [minus plus]] coherent events and (19[plus minus]7) [mu][sup [plus minus]][pi][sup [minus plus]][pi][sup 0] coherent events are extracted. For [ital E][gt]10 GeV, the coherent pion production cross section is determined to be (3.2[plus minus]0.7)[times]10[sup [minus]38] cm[sup 2] per neon nucleus whereas the coherent [rho] production cross section is (2.1[plus minus]0.8)[times]10[sup [minus]38] cm[sup 2] per neon nucleus. These cross sections and the kinematical characteristics of the coherent events at [vert bar][ital t][vert bar][lt]0.1 GeV[sup 2] are found to be in general agreement with the predictions of a model based on the hadron dominance and, in the pion case, on the partially conserved axial-vector current hypothesis. Also discussed is the coherent production of systems consisting of three pions.</abstract><cop>United States</cop><doi>10.1103/PhysRevD.47.2661</doi></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0556-2821 |
ispartof | Physical review. D, Particles and fields, 1993-04, Vol.47:7 |
issn | 0556-2821 1089-4918 |
language | eng |
recordid | cdi_osti_scitechconnect_6655253 |
source | American Physical Society Journals |
subjects | ANTINEUTRINO-NUCLEON INTERACTIONS BOSONS BUBBLE CHAMBERS CROSS SECTIONS DATA ELEMENTARY PARTICLES ELEMENTS EXPERIMENTAL DATA FLUIDS GAS TRACK DETECTORS GASES HADRONS HYDROGEN INFORMATION INTERACTIONS LEPTON-BARYON INTERACTIONS LEPTON-HADRON INTERACTIONS LEPTON-NUCLEON INTERACTIONS MEASURING INSTRUMENTS MESONS NEON NEUTRINO-NUCLEON INTERACTIONS NONMETALS NUMERICAL DATA PARTICLE INTERACTIONS PARTICLE KINEMATICS PARTICLE PRODUCTION PCAC THEORY PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PIONS PSEUDOSCALAR MESONS RADIATION DETECTORS RARE GASES RHO-770 MESONS VECTOR MESONS 662320 -- Neutrino Interactions-- (1992-) |
title | Coherent production of single pions and [rho] mesons in charged-current interactions of neutrinos and antineutrinos on neon nuclei at the Fermilab Tevatron |
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