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New Journal of Physics | 2011

Measurement of charm production in neutrino charged-current interactions

A. Kayis-Topaksu; G. Onengut; R. van Dantzig; M. de Jong; R. Oldeman; M. Guler; U. Köse; P. Tolun; M.G. Catanesi; M.T. Muciaccia; K. Winter; B. Van de Vyver; P. Vilain; G. Wilquet; B. Saitta; E. Di Capua; S. Ogawa; H. Shibuya; I.R. Hristova; T. Kawamura; D. Kolev; H. Meinhard; J. Panman; A. Rozanov; R. Tsenov; J.W.E. Uiterwijk; P. Zucchelli; J. Goldberg; M. Chikawa; J.S. Song

The nuclear emulsion target of the CHORUS detector was exposed to the wide-band neutrino beam of the CERN SPS of 27 GeV average neutrino energy from 1994 to 1997. In total, about 100 000 charged-current (CC) neutrino interactions with at least one identified muon were located in the emulsion target and fully reconstructed, using newly developed automated scanning systems. Charmed particles were searched for by a program recognizing particle decays. The observation of the decay in nuclear emulsion makes it possible to select a sample with very low background and minimal kinematical bias. In all, 2013 CC interactions with a charmed hadron candidate in the final state were selected and confirmed through visual inspection. The charm production rate induced by neutrinos relative to the CC cross-section is measured to be σ(νμN→μ−CX)/σ(CC)=(5.75 ± 0.32(stat)±0.30(syst))%. The charm production cross-section as a function of neutrino energy is also obtained. The results are in good agreement with previous measurements. The charm-quark hadronization produces the following charmed hadrons with relative fractions (in %): fD0=43.7±4.5, fΛc+=19.2±4.2, fD+=25.3±4.2 and fDs+=11.8±4.7.


Physics Letters B | 1988

Cross-sections for Neutrino Production of Charmed Particles

N. Ushida; T. Kondo; S. Tasaka; I.G. Park; J.S. Song; T. Hara; Y. Homma; Y. Tsuzuki; G. Fujioka; H. Fukushima; Y. Takahashi; S. Tatsumi; C. Yokoyama; K. Fujiwara; K. Taruma; S. Bahk; C. Kim; J. Park; D. C. Bailey; S. Conetti; P. Mercure; J. Trischuk; M. Turcotte; S. Aoki; K. Chiba; H. Fuchi; K. Hoshino; K. Kodama; R. Matsui; M. Miyanishi

Abstract We have found 122 charmed-particle decays among 3855 neutrino interactions located in the fiducial volume of a hybrid emulsion spectrometer installed in the Fermilab wide-band neutrino beam. We obtain an average relative charmed-particle production cross section of σ(ν μ → c μ − ) σ(ν μ →μ − ) =4.9 −0.6 +0.7 % , at an average neutrino energy of 22 GeV. We also obtain a production rate of σ(ν μ → c c ν μ ) σ(ν μ →ν μ ) =0.13 −0.11 +0.31 % , if we assume that there was an undetected muon, a limit of σ(ν μ → c c μ − ) σ(ν μ → c μ − ) CL ) can be obtained. Other cross section ratios and limits are also presented.


Physics Letters B | 1985

Direct observation of the decay of beauty particles into charm particles

J.P. Albanese; V. Alpe; S. Aoki; R. Arnold; Giustina Baroni; M. Barth; J.H. Bartley; Daniel Bertrand; G. Bertrand-Coremans; V. Bisi; A.C. Breslin; G. Carboni; E. Chesi; K. Chiba; G.S. Cook; M. Coupland; G. Crosetti; D.H. Davis; S. Dell'Uomo; S. Di Liberto; W. Bonnelly; B.G. Duff; M.J. Esten; D. Gamba; C. Gerke; M. Hazama; F.F. Heymann; K. Hoshino; D.C. Imrie; Y. Isokane

Abstract The associated production of a pair of beauty particles B− and B 0 by a 350 GeV π− interaction has been observed in an emulsion target inserted in an array of silicon microstrip detectors. Both beauty particles decay into charm particles, both of which are also observed to decay in the emulsion. Two negative muons were identified and their momenta measured in a large muon spectrometer. One muon has a pT of 1.9 GeV/c and is associated with a beauty particle decay. The other, with a pT of 0.45 GeV/c is associated with a charm particle decay. The flight times of the two beauty particles are respectively (0.8 ± 0.1) × 10−13 s and (5+2−1) × 10−13 s. Alternative interpretations of this event have negligible probability.


Physical Review Letters | 1980

Measurement of the D+, F+, and Lambda(c)+ Charmed Particle Lifetimes

N. Ushida; D. Pitman; M. Miyanishi; H. Shibuya; G. Fujioka; N. R. Stanton; P. Davis; J. Yokota; K. Hoshino; Y. Tsuzuki; S. Conetti; T.-S. Yoon; J. D. Prentice; Y. Noguchi; M. Teranaka; S. Bahk; C. Hebert; David Bailey; H. Fuchi; K. Niu; S. Lokanathan; J.S. Song; Yoshiyuki Takahashi; J. Trischuk; T. A. Romanowski; J. Park; H. Fukushima; P. Sinervo; B. McLeod; C. Yokoyama

From the analysis of 685 neutrino and antineutrino interactions in an emulsion target, fifteen candidates for the multiprong decay of charged charmed particles are found. This Letter presents liketimes for the D/sup + -/, F/sup + -/, and ..lambda../sub c//sup +/ states based on the fitted events of the sample.


Nuclear Instruments and Methods in Physics Research | 1984

EXPERIMENTAL DETAILS ON LIFETIME MEASUREMENTS OF NEUTRINO PRODUCED CHARMED PARTICLES IN A TAGGED EMULSION SPECTROMETER

N. Ushida; T. Kondo; G. Fujioka; H. Fukushima; Y. Takahashi; S. Tatsumi; C. Yokoyama; Y. Homma; Y. Tsuzuki; S. Bahk; C. Kim; J. Park; J. Song; D. C. Bailey; S. Conetti; J. Fisher; J. Trischuk; H. Fuchi; K. Noshino; M. Miyanishi; K. Niu; K. Niwa; H. Shibuya; Y. Yanagisawa; S. Errede; M. Gutzwiller; S. Kuramata; N.W. Reay; K. Reibel; T. A. Romanowski

Abstract A new type of hybrid appaatus, which consisted of an emulsion target and a magnet spectrometer, was successfully used in an experiment to measure lifetimes of charmed particles produced by the wide-band neutrino beam from 350 GeV protons at Fermilab. The emulsion target was essential to find short distance decay vertices andthe counter spectrometer was used both to localize the neutrino events in the emulsion and also to identify the particles from weak decays and those produced in the neutrino interactions. Newly introduced emulsion techniques such as the changeable sheet as a low background interface to couple the emulsion target with the counter spectrometer, and the single track followback method to locate interaction and decay vertices in the emulsion, were proved to be very powerful. Details of the experimental apparatus and of the method of analysis employed are described.


Physics Letters B | 1995

Production of a twin single hypernuclei and the Ξ−-nuclear interaction

S. Aoki; S.Y. Bahk; K.S. Chung; S.H. Chung; H. Funahashi; C.H. Hahn; T. Hara; S. Hirata; K. Hoshino; M. Ieiri; T. Ijima; K. Imai; Y. Itow; T. Jin-ya; M. Kazuno; K. Kikuchi; C. Kim; D.C. Kim; J. Y. Kim; K. Kodama; Y. Maeda; A. Masaike; A. Masuoka; Y. Matsuda; C. Nagoshi; M. Nakamura; S. Nakanishi; Takafumi Nakano; K. Nakazawa; K. Niwa

Abstract An event accompanied by two single hyperfragments emitted from a Ξ− nuclear capture at rest was found in a nuclear emulsion. It is interpreted as a Ξ−-12C bound system decaying into either a) Λ4H + Λ9Be, b) Λ 4 H + Λ 9 Be ∗ or c) Λ 4 H ∗ + Λ 9 Be . The binding energy of the Ξ-12C system is obtained as a) 3.70−0.19+0.18 MeV, b) 0.62−0.19+0.18 MeV and c) 2.66−0.19+0.18 MeV, respectively. The system is considered as a Ξ− hypernucleus in the cases a) and c). In case b), this event and another event of the same type (Yokohama event) can both be interpreted as a decay from the Ξ-12C system in 2P state when a shallow Ξ−-nuclear potential is assumed.


Nuclear Physics | 1990

Electromagnetic dissociation of 200 GeV/nucleon 16O and 32s ions in nuclear emulsions

G. Baroni; V. Bisi; A.C. Breslin; D.H. Davis; S. Dell'Uomo; S. Di Liberto; P. Giubellino; G. Grella; K. Hoshino; M. Kazuno; M. Kobayashi; K. Kodama; A. Marzari-Chiesa; M. A. Mazzoni; F. Meddi; M.T. Muciaccia; K. Niu; L. Ramello; G. Romano; G. Rosa; C. Sgarbi; H. Shibuya; S. Simone; D.N. Tovee; N. Ushida; C. Wilkin; S.K.C. Yuen

Abstract This work represents the results of an experimental investigation of the electromagnetic dissociation of 200 GeV/nucleon 16 O and 32 S ions in nuclear emulsions. Exclusive channels involving charged fragments have been studied as a function of the energy released, and, assuming a Weizsacker-Williams spectrum of virtual photons, there is a good agreement with results for the (γ, p) processes obtained with real photons. However, the rates found for other processes are larger, in particular for the (γ, α) on both nuclei. The values of the total integrated absorption cross sections are generally larger than those obtained from real photon experiments but the extent of the discrepancy depends strongly upon which photon results are used in the comparison.


Physics Letters B | 1983

Charmed hadron production by neutrinos

N. Ushida; T. Kondo; F. Fujioka; H. Fukushima; Y. Takahashi; S. Tatsumi; C. Yokohama; Y. Homma; Y. Tsuzuki; S. Bahk; C. Kim; J. Park; J. Song; D. C. Bailey; S. Conetti; J. Fischer; J. Trischuk; H. Fuchi; K. Hoshino; M. Miyanashi; K. Niu; K. Niwa; H. Shibuya; Y. Yanagisawa; S. Errede; M. Gutzwiller; S. Kuramata; N.W. Reay; K. Reibel; T. A. Romanowski

Abstract Charmed hadron production has been studied using a hybrid emulsion spectrometer in the Fermilab wide-band neutrino beam. The relative rates of D0, D+, F+, and Λ+c production have been measured - the fraction of D mesons is 69 ± 8 10 % . Momentum, transverse momentum, Feynman X, and fragmentation (Z) distributions are presented. The mean Z for charmed hadrons is 0.59 ± 0.03 (±0.03). Charmed target fragments have been observed.


Physics Letters B | 1988

Production characteristics of charmed particles in neutrino interactions

N. Ushida; T. Kondo; S. Tasaka; I.G. Park; J.S. Song; T. Hara; Y. Homma; Y. Tsuzuki; G. Fujioka; H. Fukushima; Y. Takahashi; S. Tatsumi; C. Yokoyama; K. Fujiwara; K. Taruma; S. Bahk; C. Kim; J. Park; D. C. Bailey; S. Conetti; P. Mercure; J. Trischuk; M. Turcotte; S. Aoki; K. Chiba; H. Fuchi; K. Hoshino; K. Kodama; R. Matsui; M. Miyanishi

Abstract Using a hybrid emulsion spectrometer installed in the Fermilab wide-band neutrino beam, we located a total of 3855 neutrino interactions in the fiducial volume of our target. For 122 charmed-particle decays found in these interactions, we present distributions of x , y , charm-muon angular projection, Feynman- X , and the fragmentation Z . We find that the number of strange quarks in the nucleon sea is 4.2±2.1±2.6% of the number of down quarks.


Nuclear Physics | 1998

Quasifree p(K-,K+)Xi- reaction in nuclear emulsion

S. Aoki; S. Asai; S.Y. Bahk; S.H. Chung; H. Funahashi; C.H. Hahn; M. Hanabata; T. Hara; K. Hoshino; M. Ieiri; M. Iida; T. Iijima; K. Imai; Y. Itow; T. Jin-ya; M. Kazuno; C. O. Kim; D.C. Kim; J. Y. Kim; Kunihiko Kodama; T. Kuze; Y. Maeda; A. Masaike; Y. Matsuda; A. Matsui; K. Murakami; C. Nagoshi; Masaki Nakamura; S. Nakanishi; Takenori Nakano

Abstract A study of 1.66 GeV c K − beam induced ( K − ,K + ) reactions in the nuclear emulsion target is presented and 796 ( K − , K + ) reaction vertices ( p K + ⩾ 1 GeV /c ) containing 18 single hyperfragments are identified. There is no clear(spatially separated) double hyperfragment nor twin single hyperfragment in the identified 796 ( K − ,K + ) reactions. These events are classified and their characteristics are described in detail. In the region p K + ⩾ 1 GeV /c where the quasifree K − (p) → K + Ξ − is the dominant process, the probability of Ξ − emission from the reaction vertex is determined to be 73.9 −4.6 +4.5 %. From this value, the mean free path of Ξ − in a nucleus is estimated to be 4.7 −1.0 +1.5 fm for 〈p Ξ − 〉 ∼ 0.6 GeV /c by assuming a simple model of uniform nuclear matter.

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