C.S. Yoon
Gyeongsang National University
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Featured researches published by C.S. Yoon.
Physics Letters B | 2001
K. Kodama; N. Ushida; C. Andreopoulos; N. Saoulidou; G. Tzanakos; P. M. Yager; B. Baller; D. J. Boehnlein; Walter Freeman; B. Lundberg; J. Morfin; R. Rameika; J. C. Yun; J.S. Song; C.S. Yoon; S.H. Chung; P. Berghaus; M. Kubantsev; Neville W. Reay; R. A. Sidwell; N.R. Stanton; S. Yoshida; S. Aoki; T. Hara; J. T. Rhee; D. P. Ciampa; C. Erickson; M. Graham; K. Heller; R. Rusack
Abstract The DONUT experiment has analyzed 203 neutrino interactions recorded in nuclear emulsion targets. A decay search has found evidence of four tau neutrino interactions with an estimated background of 0.34 events. This number is consistent with the Standard Model expectation.The DONUT experiment has analyzed 203 neutrino interactions recorded in nuclear emulsion targets. A decay search has found evidence of four tau neutrino interactions with an estimated background of 0.34 events. This number is consistent with the Standard Model expectation.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
K. Kodama; N. Saoulidou; G. Tzanakos; B. Baller; B. Lundberg; R. Rameika; J.S. Song; C.S. Yoon; S.H. Chung; S. Aoki; T. Hara; C. Erickson; K. Heller; R. Schwienhorst; J. Sielaff; J. Trammell; K. Hoshino; H. Jiko; J. Kawada; T Kawai; M. Komatsu; H Matsuoka; M. Miyanishi; M Nakamura; T. Nakano; K. Narita; K. Niwa; N. Nonaka; K. Okada; O. Sato
Abstract The DONUT experiment used an emulsion/counter-hybrid-detector, which succeeded in detecting tau–neutrino charged-current interactions. A new method of emulsion analysis, NETSCAN, was used to locate neutrino events and detect tau decays. It is based on a fully automated emulsion readout system (Ultra Track Selector) developed at Nagoya University. The achieved plate-to-plate alignment accuracy of ∼0.2 μm over an area of 2.6 mm ×2.6 mm permitted an efficient and systematic tau decay search using emulsion data. Moreover, this accuracy allowed measurement of particle momenta by multiple Coulomb scattering, and contributed to the efficient background rejection for the ν τ candidates. This paper describes details of our emulsion analysis methods.
New Journal of Physics | 2011
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 | 2001
R. Schwienhorst; D. P. Ciampa; C. Erickson; M. Graham; K. Heller; R. Rusack; J. Sielaff; J. Trammell; J. Wilcox; K. Kodama; N. Ushida; C. Andreopoulos; N. Saoulidou; G. Tzanakos; P. M. Yager; B. Baller; D. J. Boehnlein; Walter Freeman; B. Lundberg; J. Morfin; R. Rameika; J. C. Yun; J.S. Song; C.S. Yoon; S.H. Chung; P. Berghaus; M. Kubantsev; Neville W. Reay; R. A. Sidwell; N.R. Stanton
Abstract Using a neutrino beam in which a ντ component was identified for the first time, the ντ magnetic moment was measured based on a search for an anomalous increase in the number of neutrino–electron interactions. One such event was observed when 2.3 were expected from background processes, giving an upper 90% confidence limit on μντ of 3.9×10−7μB.Using a prompt neutrino beam in which a nu_tau component was identified for the first time, the nu_tau magnetic moment was measured based on a search for an anomalous increase in the number of neutrino-electron interactions. One such event was observed when 2.3 were expected from background processes, giving an upper 90% confidence limit of 3.9x10^-7 Bohr magnetons.
Physics Letters B | 1995
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 Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
S. Aoki; E. Barbuto; C. Bozza; J.P. Fabre; W Flegal; G. Grella; M Guler; T. Hara; K. Hoshino; Y. Ishii; T. Kawamura; D.C. Kim; M. Kobayashi; Y. Kotaka; T. Kozaki; F. Meddi; M.T. Muciaccia; K. Nakamura; E. Niu; Y. Obayashi; S. Ogawa; G. Romano; G. Rosa; O. Sato; V Shamanov; H. Shibuya; S. Simone; V Smirnitsky; J.S. Song; P. Tolun
Abstract We describe the (2×800 kg ) emulsion target in the CHORUS hybrid detector set-up for the search of ν μ →ν τ oscillations, together with the CERN pouring and processing facilities (upgraded for this purpose), and the techniques employed to treat the emulsions used as the active target in the experiment.
Physics Letters B | 2001
A. Ichikawa; J. K. Ahn; H. Akikawa; S. Aoki; K. Arai; S.Y. Bahk; K. M. Baik; B. Bassalleck; J.H. Chung; M. S. Chung; K. Hoshino; M. Ieiri; K. Imai; Y. H. Iwata; Y. S. Iwata; H. Kanda; M. Kaneko; T. Kawai; C. Kim; J. Y. Kim; S. J. Kim; S. H. Kim; Y. Kondo; T. Kouketsu; Y. L. Lee; J. W. C. McNabb; M. Mitsuhara; Y. Nagase; C. Nagoshi; K. Nakazawa
Abstract A hybrid emulsion experiment was carried out to study double-strangeness nuclei produced via Ξ− hyperon capture at rest with the expectation of ten times larger statistics than previous experiments. We have analyzed 5% of the total emulsion and found one “twin-hypernuclei” event involving the emission of two single-Λ hypernuclei and a nuclear fragment from a Ξ− hyperon stopping point. The event is interpreted as the decay of a Ξ − + 14 N atomic system to 5 Λ He + 5 Λ He + 4 He + neutron . The species of the Ξ−-atom and the fragmentation products are uniquely identified for the first time for twin-hypernuclei events. Combined with the results from a past hybrid-emulsion experiment, one double-Λ hypernucleus and three twin-hypernuclei events have been found from Ξ− captures on light emulsion nuclei. The ratio of the detected rate of double-Λ hypernuclei to that of twin-hypernuclei is compared with theoretical estimates.
Physics Letters B | 1996
K. Kodama; S Torikai; N. Ushida; A. Mokhtarani; V.S. Paolone; J.T. Volk; J.O. Wilcox; P. M. Yager; R.M. Edelstein; A.P. Freyberger; D.B. Gibaut; Richard Lipton; W.R. Nichols; D.M. Potter; J. Russ; C. Zhang; Y. Zhang; H.I. Jang; J. Y. Kim; B. Baller; R. Stefanski; K. Nakazawa; S.H. Chung; M.S. Park; I.G. Park; J.S. Song; C.S. Yoon; M. Aryal; N. W. Reay; R. A. Sidwell
We have observed
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1994
K. Kodama; N. Ushida; A. Mokhtarani; V.S. Paolone; J.T. Volk; J.O. Wilcox; P. M. Yager; R.M. Edelstein; A.P. Freyberger; D.B. Gibaut; Richard Lipton; W.R. Nichols; D.M. Potter; J. Russ; C. Zhang; Y. Zhang; H.I. Jang; J. Y. Kim; T.I. Kim; I. T. Lim; M.Y. Pac; B. Baller; R. Stefanski; K. Nakazawa; K.S. Chung; S.H. Chung; D.C. Kim; I.G. Park; M.S. Park; J.S. Song
23.2 \pm 6.0_{-0.9}^{+1.0}
In: Cheon, IT and Choi, T and Hong, SW and Lee, SH, (eds.) HADRONS AND NUCLEI. (pp. 180 - 188). AMER INST PHYSICS (2001) | 2002
J. K. Ahn; Y. Akaishi; H. Akikawa; S. Aoki; K. Arai; S.Y. Bahk; K. M. Baik; B. Bassalleck; J. H. Chung; M. S. Chung; D.H. Davis; G. B. Franklin; T. Fukuda; K. Hoshino; A. Ichikawa; M. Ieiri; K. Imai; Y. H. Iwata; Y. S. Iwata; H. Kanda; M. Kaneko; T. Kawai; C. O. Kim; J. Y. Kim; S. J. Kim; Sang-Hoon Kim; Y. Kondo; T. Kouketsu; Y. L. Lee; J. W. C. McNabb
purely-leptonic decays of