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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Veröffentlicht in:Physical review. D, Particles and fields Particles and fields, 1993-04, Vol.47:7
Hauptverfasser: 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.
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container_title Physical review. D, Particles and fields
container_volume 47:7
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. 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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>
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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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