Neutrino production of dimuons
Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinema...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1987 |
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| Umfang: |
21 |
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| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
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| Übergeordnetes Werk: |
in: The European physical journal - 1998, 33(1987) vom: Apr., Seite 483-503 |
| Übergeordnetes Werk: |
volume:33 ; year:1987 ; month:04 ; pages:483-503 ; extent:21 |
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|---|
| Katalog-ID: |
NLEJ206233205 |
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| 008 | 070528s1987 xx |||||o 00| ||eng c | ||
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| 041 | |a eng | ||
| 245 | 1 | 0 | |a Neutrino production of dimuons |
| 264 | 1 | |c 1987 | |
| 300 | |a 21 | ||
| 336 | |a nicht spezifiziert |b zzz |2 rdacontent | ||
| 337 | |a nicht spezifiziert |b z |2 rdamedia | ||
| 338 | |a nicht spezifiziert |b zu |2 rdacarrier | ||
| 520 | |a Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. | ||
| 533 | |f Springer Online Journal Archives 1860-2002 | ||
| 700 | 1 | |a Lang, K. |4 oth | |
| 700 | 1 | |a Bodek, A. |4 oth | |
| 700 | 1 | |a Borcherding, F. |4 oth | |
| 700 | 1 | |a Giokaris, N. |4 oth | |
| 700 | 1 | |a Stockdale, I. E. |4 oth | |
| 700 | 1 | |a Auchincloss, P. |4 oth | |
| 700 | 1 | |a Blair, R. |4 oth | |
| 700 | 1 | |a Haber, C. |4 oth | |
| 700 | 1 | |a Mishra, S. |4 oth | |
| 700 | 1 | |a Oltman, E. |4 oth | |
| 700 | 1 | |a Ruiz, M. |4 oth | |
| 700 | 1 | |a Sciulli, F. J. |4 oth | |
| 700 | 1 | |a Shaevitz, M. |4 oth | |
| 700 | 1 | |a Smith, W. H. |4 oth | |
| 700 | 1 | |a Zhu, R. |4 oth | |
| 700 | 1 | |a Chu, Y. K. |4 oth | |
| 700 | 1 | |a MacFarlane, D. B. |4 oth | |
| 700 | 1 | |a Messner, R. L. |4 oth | |
| 700 | 1 | |a Novikoff, D. B. |4 oth | |
| 700 | 1 | |a Purohit, M. V. |4 oth | |
| 700 | 1 | |a Garfinkle, D. |4 oth | |
| 700 | 1 | |a Merritt, F. S. |4 oth | |
| 700 | 1 | |a Oreglia, M. |4 oth | |
| 700 | 1 | |a Reutens, P. |4 oth | |
| 700 | 1 | |a Coleman, R. |4 oth | |
| 700 | 1 | |a Fisk, H. E. |4 oth | |
| 700 | 1 | |a Fukushima, Y. |4 oth | |
| 700 | 1 | |a Kerns, O. |4 oth | |
| 700 | 1 | |a Jin, B. |4 oth | |
| 700 | 1 | |a Levinthal, D. |4 oth | |
| 700 | 1 | |a Kondo, T. |4 oth | |
| 700 | 1 | |a Marsh, W. |4 oth | |
| 700 | 1 | |a Rapidis, P. A. |4 oth | |
| 700 | 1 | |a Segler, S. |4 oth | |
| 700 | 1 | |a Stefanski, R. |4 oth | |
| 700 | 1 | |a Theriot, D. |4 oth | |
| 700 | 1 | |a White, H. B. |4 oth | |
| 700 | 1 | |a Yovanovitch, D. |4 oth | |
| 700 | 1 | |a Fackler, O. |4 oth | |
| 700 | 1 | |a Jenkins, K. |4 oth | |
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(DE-627)NLEJ206233205 DE-627 ger DE-627 rakwb eng Neutrino production of dimuons 1987 21 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. Springer Online Journal Archives 1860-2002 Lang, K. oth Bodek, A. oth Borcherding, F. oth Giokaris, N. oth Stockdale, I. E. oth Auchincloss, P. oth Blair, R. oth Haber, C. oth Mishra, S. oth Oltman, E. oth Ruiz, M. oth Sciulli, F. J. oth Shaevitz, M. oth Smith, W. H. oth Zhu, R. oth Chu, Y. K. oth MacFarlane, D. B. oth Messner, R. L. oth Novikoff, D. B. oth Purohit, M. V. oth Garfinkle, D. oth Merritt, F. S. oth Oreglia, M. oth Reutens, P. oth Coleman, R. oth Fisk, H. E. oth Fukushima, Y. oth Kerns, O. oth Jin, B. oth Levinthal, D. oth Kondo, T. oth Marsh, W. oth Rapidis, P. A. oth Segler, S. oth Stefanski, R. oth Theriot, D. oth White, H. B. oth Yovanovitch, D. oth Fackler, O. oth Jenkins, K. oth in The European physical journal 1998 33(1987) vom: Apr., Seite 483-503 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:33 year:1987 month:04 pages:483-503 extent:21 http://dx.doi.org/10.1007/BF01548260 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 33 1987 4 483-503 21 |
| spelling |
(DE-627)NLEJ206233205 DE-627 ger DE-627 rakwb eng Neutrino production of dimuons 1987 21 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. Springer Online Journal Archives 1860-2002 Lang, K. oth Bodek, A. oth Borcherding, F. oth Giokaris, N. oth Stockdale, I. E. oth Auchincloss, P. oth Blair, R. oth Haber, C. oth Mishra, S. oth Oltman, E. oth Ruiz, M. oth Sciulli, F. J. oth Shaevitz, M. oth Smith, W. H. oth Zhu, R. oth Chu, Y. K. oth MacFarlane, D. B. oth Messner, R. L. oth Novikoff, D. B. oth Purohit, M. V. oth Garfinkle, D. oth Merritt, F. S. oth Oreglia, M. oth Reutens, P. oth Coleman, R. oth Fisk, H. E. oth Fukushima, Y. oth Kerns, O. oth Jin, B. oth Levinthal, D. oth Kondo, T. oth Marsh, W. oth Rapidis, P. A. oth Segler, S. oth Stefanski, R. oth Theriot, D. oth White, H. B. oth Yovanovitch, D. oth Fackler, O. oth Jenkins, K. oth in The European physical journal 1998 33(1987) vom: Apr., Seite 483-503 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:33 year:1987 month:04 pages:483-503 extent:21 http://dx.doi.org/10.1007/BF01548260 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 33 1987 4 483-503 21 |
| allfields_unstemmed |
(DE-627)NLEJ206233205 DE-627 ger DE-627 rakwb eng Neutrino production of dimuons 1987 21 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. Springer Online Journal Archives 1860-2002 Lang, K. oth Bodek, A. oth Borcherding, F. oth Giokaris, N. oth Stockdale, I. E. oth Auchincloss, P. oth Blair, R. oth Haber, C. oth Mishra, S. oth Oltman, E. oth Ruiz, M. oth Sciulli, F. J. oth Shaevitz, M. oth Smith, W. H. oth Zhu, R. oth Chu, Y. K. oth MacFarlane, D. B. oth Messner, R. L. oth Novikoff, D. B. oth Purohit, M. V. oth Garfinkle, D. oth Merritt, F. S. oth Oreglia, M. oth Reutens, P. oth Coleman, R. oth Fisk, H. E. oth Fukushima, Y. oth Kerns, O. oth Jin, B. oth Levinthal, D. oth Kondo, T. oth Marsh, W. oth Rapidis, P. A. oth Segler, S. oth Stefanski, R. oth Theriot, D. oth White, H. B. oth Yovanovitch, D. oth Fackler, O. oth Jenkins, K. oth in The European physical journal 1998 33(1987) vom: Apr., Seite 483-503 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:33 year:1987 month:04 pages:483-503 extent:21 http://dx.doi.org/10.1007/BF01548260 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 33 1987 4 483-503 21 |
| allfieldsGer |
(DE-627)NLEJ206233205 DE-627 ger DE-627 rakwb eng Neutrino production of dimuons 1987 21 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. Springer Online Journal Archives 1860-2002 Lang, K. oth Bodek, A. oth Borcherding, F. oth Giokaris, N. oth Stockdale, I. E. oth Auchincloss, P. oth Blair, R. oth Haber, C. oth Mishra, S. oth Oltman, E. oth Ruiz, M. oth Sciulli, F. J. oth Shaevitz, M. oth Smith, W. H. oth Zhu, R. oth Chu, Y. K. oth MacFarlane, D. B. oth Messner, R. L. oth Novikoff, D. B. oth Purohit, M. V. oth Garfinkle, D. oth Merritt, F. S. oth Oreglia, M. oth Reutens, P. oth Coleman, R. oth Fisk, H. E. oth Fukushima, Y. oth Kerns, O. oth Jin, B. oth Levinthal, D. oth Kondo, T. oth Marsh, W. oth Rapidis, P. A. oth Segler, S. oth Stefanski, R. oth Theriot, D. oth White, H. B. oth Yovanovitch, D. oth Fackler, O. oth Jenkins, K. oth in The European physical journal 1998 33(1987) vom: Apr., Seite 483-503 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:33 year:1987 month:04 pages:483-503 extent:21 http://dx.doi.org/10.1007/BF01548260 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 33 1987 4 483-503 21 |
| allfieldsSound |
(DE-627)NLEJ206233205 DE-627 ger DE-627 rakwb eng Neutrino production of dimuons 1987 21 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. Springer Online Journal Archives 1860-2002 Lang, K. oth Bodek, A. oth Borcherding, F. oth Giokaris, N. oth Stockdale, I. E. oth Auchincloss, P. oth Blair, R. oth Haber, C. oth Mishra, S. oth Oltman, E. oth Ruiz, M. oth Sciulli, F. J. oth Shaevitz, M. oth Smith, W. H. oth Zhu, R. oth Chu, Y. K. oth MacFarlane, D. B. oth Messner, R. L. oth Novikoff, D. B. oth Purohit, M. V. oth Garfinkle, D. oth Merritt, F. S. oth Oreglia, M. oth Reutens, P. oth Coleman, R. oth Fisk, H. E. oth Fukushima, Y. oth Kerns, O. oth Jin, B. oth Levinthal, D. oth Kondo, T. oth Marsh, W. oth Rapidis, P. A. oth Segler, S. oth Stefanski, R. oth Theriot, D. oth White, H. B. oth Yovanovitch, D. oth Fackler, O. oth Jenkins, K. oth in The European physical journal 1998 33(1987) vom: Apr., Seite 483-503 (DE-627)NLEJ188986553 (DE-600)1459069-4 1434-6052 nnns volume:33 year:1987 month:04 pages:483-503 extent:21 http://dx.doi.org/10.1007/BF01548260 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 33 1987 4 483-503 21 |
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Lang, K. @@oth@@ Bodek, A. @@oth@@ Borcherding, F. @@oth@@ Giokaris, N. @@oth@@ Stockdale, I. E. @@oth@@ Auchincloss, P. @@oth@@ Blair, R. @@oth@@ Haber, C. @@oth@@ Mishra, S. @@oth@@ Oltman, E. @@oth@@ Ruiz, M. @@oth@@ Sciulli, F. J. @@oth@@ Shaevitz, M. @@oth@@ Smith, W. H. @@oth@@ Zhu, R. @@oth@@ Chu, Y. K. @@oth@@ MacFarlane, D. B. @@oth@@ Messner, R. L. @@oth@@ Novikoff, D. B. @@oth@@ Purohit, M. V. @@oth@@ Garfinkle, D. @@oth@@ Merritt, F. S. @@oth@@ Oreglia, M. @@oth@@ Reutens, P. @@oth@@ Coleman, R. @@oth@@ Fisk, H. E. @@oth@@ Fukushima, Y. @@oth@@ Kerns, O. @@oth@@ Jin, B. @@oth@@ Levinthal, D. @@oth@@ Kondo, T. @@oth@@ Marsh, W. @@oth@@ Rapidis, P. A. @@oth@@ Segler, S. @@oth@@ Stefanski, R. @@oth@@ Theriot, D. @@oth@@ White, H. B. @@oth@@ Yovanovitch, D. @@oth@@ Fackler, O. @@oth@@ Jenkins, K. @@oth@@ |
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A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Springer Online Journal Archives 1860-2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lang, K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Bodek, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Borcherding, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Giokaris, N.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Stockdale, I. 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Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. |
| abstractGer |
Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. |
| abstract_unstemmed |
Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data. |
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Lang, K. Bodek, A. Borcherding, F. Giokaris, N. Stockdale, I. E. Auchincloss, P. Blair, R. Haber, C. Mishra, S. Oltman, E. Ruiz, M. Sciulli, F. J. Shaevitz, M. Smith, W. H. Zhu, R. Chu, Y. K. MacFarlane, D. B. Messner, R. L. Novikoff, D. B. Purohit, M. V. Garfinkle, D. Merritt, F. S. Oreglia, M. Reutens, P. Coleman, R. Fisk, H. E. Fukushima, Y. Kerns, O. Jin, B. Levinthal, D. Kondo, T. Marsh, W. Rapidis, P. A. Segler, S. Stefanski, R. Theriot, D. White, H. B. Yovanovitch, D. Fackler, O. Jenkins, K. |
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Lang, K. Bodek, A. Borcherding, F. Giokaris, N. Stockdale, I. E. Auchincloss, P. Blair, R. Haber, C. Mishra, S. Oltman, E. Ruiz, M. Sciulli, F. J. Shaevitz, M. Smith, W. H. Zhu, R. Chu, Y. K. MacFarlane, D. B. Messner, R. L. Novikoff, D. B. Purohit, M. V. Garfinkle, D. Merritt, F. S. Oreglia, M. Reutens, P. Coleman, R. Fisk, H. E. Fukushima, Y. Kerns, O. Jin, B. Levinthal, D. Kondo, T. Marsh, W. Rapidis, P. A. Segler, S. Stefanski, R. Theriot, D. White, H. B. Yovanovitch, D. Fackler, O. Jenkins, K. |
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A sample of 18v μ like sign dimuon events withP μ>9 GeV/c yields 6.6±4.8 events after backgroud subtraction and a prompt rate of (1.0±0.7)×10−4 per single muon event. The kinematics of these events are compared with those of the non-prompt sources. A total of 437v μ and 31 $$\bar v_\mu $$ opposite sign dimuon events withP μ>4.3 GeV/c are used to measure the strange quark content of the nucleon: $$\kappa = {{2s} \mathord{\left/ {\vphantom {{2s} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}} \right. \kern-\nulldelimiterspace} {\left( {\bar u + \bar d} \right) = 0.52_{ - 0.15}^{ + 0.17} \left( {or\eta _s \frac{{2s}}{{u + d}} = 0.075 \pm 0.019} \right) for 100< E_v< 230 GeV\left( {\left\langle {Q^2 } \right\rangle = {{23 GeV^2 } \mathord{\left/ {\vphantom {{23 GeV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}} \right)}}$$ using a charm semileptonic branching ratio of (10.9±1.4)% extracted from measurements ine + e − collisions and neutrino emulsion data.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Springer Online Journal Archives 1860-2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lang, K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Bodek, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Borcherding, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Giokaris, N.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Stockdale, I. 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J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Shaevitz, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Smith, W. H.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zhu, R.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Chu, Y. K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">MacFarlane, D. B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Messner, R. L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Novikoff, D. B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Purohit, M. V.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Garfinkle, D.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Merritt, F. S.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Oreglia, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Reutens, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Coleman, R.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fisk, H. E.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fukushima, Y.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kerns, O.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jin, B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Levinthal, D.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kondo, T.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Marsh, W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Rapidis, P. A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Segler, S.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Stefanski, R.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Theriot, D.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">White, H. B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Yovanovitch, D.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fackler, O.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jenkins, K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">The European physical journal</subfield><subfield code="d">1998</subfield><subfield code="g">33(1987) vom: Apr., Seite 483-503</subfield><subfield code="w">(DE-627)NLEJ188986553</subfield><subfield code="w">(DE-600)1459069-4</subfield><subfield code="x">1434-6052</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:33</subfield><subfield code="g">year:1987</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:483-503</subfield><subfield code="g">extent:21</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://dx.doi.org/10.1007/BF01548260</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SOJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">33</subfield><subfield code="j">1987</subfield><subfield code="c">4</subfield><subfield code="h">483-503</subfield><subfield code="g">21</subfield></datafield></record></collection>
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