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 18vμ like sign dimuon events withPμ>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 k...
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Autor*in:	Lang, K. [verfasserIn] 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.

Format:	Artikel
Sprache:	Englisch

Erschienen:	1987

Schlagwörter:	Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band

Anmerkung:	© Springer-Verlag 1987

Übergeordnetes Werk:	Enthalten in: Zeitschrift für Physik - Springer-Verlag, 1979, 33(1987), 4 vom: Dez., Seite 483-503
Übergeordnetes Werk:	volume:33 ; year:1987 ; number:4 ; month:12 ; pages:483-503

Links:	Volltext

DOI / URN:	10.1007/BF01548260

Katalog-ID:	OLC2091898066

Internformat


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100	1		\|a Lang, K. \|e verfasserin \|4 aut
245	1	0	\|a Neutrino production of dimuons
264		1	\|c 1987
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520			\|a Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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.
650		4	\|a Field Theory
650		4	\|a Elementary Particle
650		4	\|a Quantum Field Theory
650		4	\|a Opposite Sign
650		4	\|a Narrow Band
700	1		\|a Bodek, A. \|4 aut
700	1		\|a Borcherding, F. \|4 aut
700	1		\|a Giokaris, N. \|4 aut
700	1		\|a Stockdale, I. E. \|4 aut
700	1		\|a Auchincloss, P. \|4 aut
700	1		\|a Blair, R. \|4 aut
700	1		\|a Haber, C. \|4 aut
700	1		\|a Mishra, S. \|4 aut
700	1		\|a Oltman, E. \|4 aut
700	1		\|a Ruiz, M. \|4 aut
700	1		\|a Sciulli, F. J. \|4 aut
700	1		\|a Shaevitz, M. \|4 aut
700	1		\|a Smith, W. H. \|4 aut
700	1		\|a Zhu, R. \|4 aut
700	1		\|a Chu, Y. K. \|4 aut
700	1		\|a MacFarlane, D. B. \|4 aut
700	1		\|a Messner, R. L. \|4 aut
700	1		\|a Novikoff, D. B. \|4 aut
700	1		\|a Purohit, M. V. \|4 aut
700	1		\|a Garfinkle, D. \|4 aut
700	1		\|a Merritt, F. S. \|4 aut
700	1		\|a Oreglia, M. \|4 aut
700	1		\|a Reutens, P. \|4 aut
700	1		\|a Coleman, R. \|4 aut
700	1		\|a Fisk, H. E. \|4 aut
700	1		\|a Fukushima, Y. \|4 aut
700	1		\|a Kerns, O. \|4 aut
700	1		\|a Jin, B. \|4 aut
700	1		\|a Levinthal, D. \|4 aut
700	1		\|a Kondo, T. \|4 aut
700	1		\|a Marsh, W. \|4 aut
700	1		\|a Rapidis, P. A. \|4 aut
700	1		\|a Segler, S. \|4 aut
700	1		\|a Stefanski, R. \|4 aut
700	1		\|a Theriot, D. \|4 aut
700	1		\|a White, H. B. \|4 aut
700	1		\|a Yovanovitch, D. \|4 aut
700	1		\|a Fackler, O. \|4 aut
700	1		\|a Jenkins, K. \|4 aut
773	0	8	\|i Enthalten in \|t Zeitschrift für Physik \|d Springer-Verlag, 1979 \|g 33(1987), 4 vom: Dez., Seite 483-503 \|w (DE-627)130618799 \|w (DE-600)795252-1 \|w (DE-576)016125487 \|x 0170-9739 \|7 nnns
773	1	8	\|g volume:33 \|g year:1987 \|g number:4 \|g month:12 \|g pages:483-503
856	4	1	\|u https://doi.org/10.1007/BF01548260 \|z lizenzpflichtig \|3 Volltext
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912			\|a GBV_ILN_21
912			\|a GBV_ILN_22
912			\|a GBV_ILN_30
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912			\|a GBV_ILN_70
912			\|a GBV_ILN_130
912			\|a GBV_ILN_267
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2012
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2018
912			\|a GBV_ILN_2409
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4082
912			\|a GBV_ILN_4103
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4310
912			\|a GBV_ILN_4315
912			\|a GBV_ILN_4319
912			\|a GBV_ILN_4323
951			\|a AR
952			\|d 33 \|j 1987 \|e 4 \|c 12 \|h 483-503

Indexfelder

author_variant	k l kl a b ab f b fb n g ng i e s ie ies p a pa r b rb c h ch s m sm e o eo m r mr f j s fj fjs m s ms w h s wh whs r z rz y k c yk ykc d b m db dbm r l m rl rlm d b n db dbn m v p mv mvp d g dg f s m fs fsm m o mo p r pr r c rc h e f he hef y f yf o k ok b j bj d l dl t k tk w m wm p a r pa par s s ss r s rs d t dt h b w hb hbw d y dy o f of k j kj
matchkey_str	article:01709739:1987----::etiordcin
hierarchy_sort_str	1987
publishDate	1987
allfields	10.1007/BF01548260 doi (DE-627)OLC2091898066 (DE-He213)BF01548260-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Lang, K. verfasserin aut Neutrino production of dimuons 1987 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1987 Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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. Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band Bodek, A. aut Borcherding, F. aut Giokaris, N. aut Stockdale, I. E. aut Auchincloss, P. aut Blair, R. aut Haber, C. aut Mishra, S. aut Oltman, E. aut Ruiz, M. aut Sciulli, F. J. aut Shaevitz, M. aut Smith, W. H. aut Zhu, R. aut Chu, Y. K. aut MacFarlane, D. B. aut Messner, R. L. aut Novikoff, D. B. aut Purohit, M. V. aut Garfinkle, D. aut Merritt, F. S. aut Oreglia, M. aut Reutens, P. aut Coleman, R. aut Fisk, H. E. aut Fukushima, Y. aut Kerns, O. aut Jin, B. aut Levinthal, D. aut Kondo, T. aut Marsh, W. aut Rapidis, P. A. aut Segler, S. aut Stefanski, R. aut Theriot, D. aut White, H. B. aut Yovanovitch, D. aut Fackler, O. aut Jenkins, K. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1979 33(1987), 4 vom: Dez., Seite 483-503 (DE-627)130618799 (DE-600)795252-1 (DE-576)016125487 0170-9739 nnns volume:33 year:1987 number:4 month:12 pages:483-503 https://doi.org/10.1007/BF01548260 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 AR 33 1987 4 12 483-503
spelling	10.1007/BF01548260 doi (DE-627)OLC2091898066 (DE-He213)BF01548260-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Lang, K. verfasserin aut Neutrino production of dimuons 1987 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1987 Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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. Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band Bodek, A. aut Borcherding, F. aut Giokaris, N. aut Stockdale, I. E. aut Auchincloss, P. aut Blair, R. aut Haber, C. aut Mishra, S. aut Oltman, E. aut Ruiz, M. aut Sciulli, F. J. aut Shaevitz, M. aut Smith, W. H. aut Zhu, R. aut Chu, Y. K. aut MacFarlane, D. B. aut Messner, R. L. aut Novikoff, D. B. aut Purohit, M. V. aut Garfinkle, D. aut Merritt, F. S. aut Oreglia, M. aut Reutens, P. aut Coleman, R. aut Fisk, H. E. aut Fukushima, Y. aut Kerns, O. aut Jin, B. aut Levinthal, D. aut Kondo, T. aut Marsh, W. aut Rapidis, P. A. aut Segler, S. aut Stefanski, R. aut Theriot, D. aut White, H. B. aut Yovanovitch, D. aut Fackler, O. aut Jenkins, K. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1979 33(1987), 4 vom: Dez., Seite 483-503 (DE-627)130618799 (DE-600)795252-1 (DE-576)016125487 0170-9739 nnns volume:33 year:1987 number:4 month:12 pages:483-503 https://doi.org/10.1007/BF01548260 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 AR 33 1987 4 12 483-503
allfields_unstemmed	10.1007/BF01548260 doi (DE-627)OLC2091898066 (DE-He213)BF01548260-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Lang, K. verfasserin aut Neutrino production of dimuons 1987 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1987 Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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. Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band Bodek, A. aut Borcherding, F. aut Giokaris, N. aut Stockdale, I. E. aut Auchincloss, P. aut Blair, R. aut Haber, C. aut Mishra, S. aut Oltman, E. aut Ruiz, M. aut Sciulli, F. J. aut Shaevitz, M. aut Smith, W. H. aut Zhu, R. aut Chu, Y. K. aut MacFarlane, D. B. aut Messner, R. L. aut Novikoff, D. B. aut Purohit, M. V. aut Garfinkle, D. aut Merritt, F. S. aut Oreglia, M. aut Reutens, P. aut Coleman, R. aut Fisk, H. E. aut Fukushima, Y. aut Kerns, O. aut Jin, B. aut Levinthal, D. aut Kondo, T. aut Marsh, W. aut Rapidis, P. A. aut Segler, S. aut Stefanski, R. aut Theriot, D. aut White, H. B. aut Yovanovitch, D. aut Fackler, O. aut Jenkins, K. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1979 33(1987), 4 vom: Dez., Seite 483-503 (DE-627)130618799 (DE-600)795252-1 (DE-576)016125487 0170-9739 nnns volume:33 year:1987 number:4 month:12 pages:483-503 https://doi.org/10.1007/BF01548260 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 AR 33 1987 4 12 483-503
allfieldsGer	10.1007/BF01548260 doi (DE-627)OLC2091898066 (DE-He213)BF01548260-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Lang, K. verfasserin aut Neutrino production of dimuons 1987 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1987 Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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. Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band Bodek, A. aut Borcherding, F. aut Giokaris, N. aut Stockdale, I. E. aut Auchincloss, P. aut Blair, R. aut Haber, C. aut Mishra, S. aut Oltman, E. aut Ruiz, M. aut Sciulli, F. J. aut Shaevitz, M. aut Smith, W. H. aut Zhu, R. aut Chu, Y. K. aut MacFarlane, D. B. aut Messner, R. L. aut Novikoff, D. B. aut Purohit, M. V. aut Garfinkle, D. aut Merritt, F. S. aut Oreglia, M. aut Reutens, P. aut Coleman, R. aut Fisk, H. E. aut Fukushima, Y. aut Kerns, O. aut Jin, B. aut Levinthal, D. aut Kondo, T. aut Marsh, W. aut Rapidis, P. A. aut Segler, S. aut Stefanski, R. aut Theriot, D. aut White, H. B. aut Yovanovitch, D. aut Fackler, O. aut Jenkins, K. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1979 33(1987), 4 vom: Dez., Seite 483-503 (DE-627)130618799 (DE-600)795252-1 (DE-576)016125487 0170-9739 nnns volume:33 year:1987 number:4 month:12 pages:483-503 https://doi.org/10.1007/BF01548260 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 AR 33 1987 4 12 483-503
allfieldsSound	10.1007/BF01548260 doi (DE-627)OLC2091898066 (DE-He213)BF01548260-p DE-627 ger DE-627 rakwb eng 530 VZ 530 VZ Lang, K. verfasserin aut Neutrino production of dimuons 1987 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1987 Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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. Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band Bodek, A. aut Borcherding, F. aut Giokaris, N. aut Stockdale, I. E. aut Auchincloss, P. aut Blair, R. aut Haber, C. aut Mishra, S. aut Oltman, E. aut Ruiz, M. aut Sciulli, F. J. aut Shaevitz, M. aut Smith, W. H. aut Zhu, R. aut Chu, Y. K. aut MacFarlane, D. B. aut Messner, R. L. aut Novikoff, D. B. aut Purohit, M. V. aut Garfinkle, D. aut Merritt, F. S. aut Oreglia, M. aut Reutens, P. aut Coleman, R. aut Fisk, H. E. aut Fukushima, Y. aut Kerns, O. aut Jin, B. aut Levinthal, D. aut Kondo, T. aut Marsh, W. aut Rapidis, P. A. aut Segler, S. aut Stefanski, R. aut Theriot, D. aut White, H. B. aut Yovanovitch, D. aut Fackler, O. aut Jenkins, K. aut Enthalten in Zeitschrift für Physik Springer-Verlag, 1979 33(1987), 4 vom: Dez., Seite 483-503 (DE-627)130618799 (DE-600)795252-1 (DE-576)016125487 0170-9739 nnns volume:33 year:1987 number:4 month:12 pages:483-503 https://doi.org/10.1007/BF01548260 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_267 GBV_ILN_2006 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2409 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 AR 33 1987 4 12 483-503
language	English
source	Enthalten in Zeitschrift für Physik 33(1987), 4 vom: Dez., Seite 483-503 volume:33 year:1987 number:4 month:12 pages:483-503
sourceStr	Enthalten in Zeitschrift für Physik 33(1987), 4 vom: Dez., Seite 483-503 volume:33 year:1987 number:4 month:12 pages:483-503
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Field Theory Elementary Particle Quantum Field Theory Opposite Sign Narrow Band
dewey-raw	530
isfreeaccess_bool	false
container_title	Zeitschrift für Physik
authorswithroles_txt_mv	Lang, K. @@aut@@ Bodek, A. @@aut@@ Borcherding, F. @@aut@@ Giokaris, N. @@aut@@ Stockdale, I. E. @@aut@@ Auchincloss, P. @@aut@@ Blair, R. @@aut@@ Haber, C. @@aut@@ Mishra, S. @@aut@@ Oltman, E. @@aut@@ Ruiz, M. @@aut@@ Sciulli, F. J. @@aut@@ Shaevitz, M. @@aut@@ Smith, W. H. @@aut@@ Zhu, R. @@aut@@ Chu, Y. K. @@aut@@ MacFarlane, D. B. @@aut@@ Messner, R. L. @@aut@@ Novikoff, D. B. @@aut@@ Purohit, M. V. @@aut@@ Garfinkle, D. @@aut@@ Merritt, F. S. @@aut@@ Oreglia, M. @@aut@@ Reutens, P. @@aut@@ Coleman, R. @@aut@@ Fisk, H. E. @@aut@@ Fukushima, Y. @@aut@@ Kerns, O. @@aut@@ Jin, B. @@aut@@ Levinthal, D. @@aut@@ Kondo, T. @@aut@@ Marsh, W. @@aut@@ Rapidis, P. A. @@aut@@ Segler, S. @@aut@@ Stefanski, R. @@aut@@ Theriot, D. @@aut@@ White, H. B. @@aut@@ Yovanovitch, D. @@aut@@ Fackler, O. @@aut@@ Jenkins, K. @@aut@@
publishDateDaySort_date	1987-12-01T00:00:00Z
hierarchy_top_id	130618799
dewey-sort	3530
id	OLC2091898066
language_de	englisch
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A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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="650" ind1=" " ind2="4"><subfield code="a">Field Theory</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Elementary Particle</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Quantum Field Theory</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Opposite Sign</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Narrow Band</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Bodek, A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Borcherding, F.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Giokaris, N.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Stockdale, I. 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author	Lang, K.
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title	Neutrino production of dimuons
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title_full	Neutrino production of dimuons
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author_browse	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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author-letter	Lang, K.
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title_sort	neutrino production of dimuons
title_auth	Neutrino production of dimuons
abstract	Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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-Verlag 1987
abstractGer	Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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-Verlag 1987
abstract_unstemmed	Abstract Neutrino interactions with two muons in the final state have been studied using the Fermilab narrow band beam. A sample of 18vμ like sign dimuon events withPμ>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 437vμ and 31$$\bar v_\mu $$ opposite sign dimuon events withPμ>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-Verlag 1987
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title_short	Neutrino production of dimuons
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author2	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.
author2Str	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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