A. Ono
Kobe University
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Featured researches published by A. Ono.
Physics Letters B | 1987
Hajime Yoshida; Y. Chiba; I. Endo; I. Hayashibara; T. Ohsugi; A. Taketani; R. Tanaka; K. Amako; Y. Arai; Herbert Friedrich Boerner; M. Fukawa; Y. Fukushima; N. Ishihara; J. Kanzaki; T. Kondo; Keisuke Maehata; T. Matsui; S. Odaka; K. Ogawa; T. Ohama; H. Sakamoto; M. Sakuda; J. Shirai; T. Sumiyoshi; F. Suekane; Y. Teramoto; F. Takasaki; T. Tsuboyama; S. Uehara; Yoshinobu Unno
Abstract The total cross section for the process of the e+e- annihilation into hadrons has been measured at the centre-of-mass energies of 50 GeV and 52 GeV and a search has been made for new heavy quarks. The ratios R = σ(e+e- → hadrons)/σpoint(e+e- → μ+μ-) obtained are 4.4±0.5 at 50 GeV and 4.7±0.3 at 52 GeV, respectively. An additional systematic uncertainty is 10%. From the event shape analysis we found no evidence for a new quark with charge 2 3 e .
Physics Letters B | 1997
H. Hamasaki; K. Abe; K. Amako; Y. Arai; Y. Asano; M. Chiba; Y. Chiba; Motomasa Daigo; M. Fukawa; Y. Fukushima; J. Haba; H. Hanai; Y. Hemmi; M. Higuchi; T. Hirose; Y. Homma; N. Ishihara; Y. Iwata; J. Kanzaki; R. Kikuchi; T. Kondo; T. T. Korhonen; H. Kurashige; E. K. Matsuda; T. Matsui; K. Miyake; S. Mori; Y. Nagashima; Y. Nakagawa; Takashi Nakamura
Abstract The cross section of the γγ → p p reaction was measured at two-photon center-of-mass energy (Wγγ) between 2.2 and 3.3 GeV, using the two-photon process at an e+e− collider, TRISTAN. The Wγγ dependence of the cross section integrated over a c.m. angular region of | cos θ ∗ | is in good agreement with the previous measurements and the theoreticalv prediction based on diquark model in the high Wγγ region.
Physics Letters B | 1990
K. Abe; K. Amako; Y. Arai; Y. Asano; Masami Chiba; Y. Chiba; M. Daigo; T. Emura; I. Endo; M. Fukawa; T. Fukui; Y. Fukushima; J. Haba; D. Haidt; I. Hayashibara; Y. Hemmi; M. Higuchi; T. Hirose; Y. Hojyo; Y. Homma; Y. Hoshi; Y. Ikegami; N. Ishihara; T. Kamitani; Nobuyuki Kanematsu; J. Kanzaki; R. Kikuchi; T. Kondo; T. Koseki; H. Kurashige
Abstract We accumulated e+e− annihilations into multi-hadrons at CM energies between 54.0 and 61.4 GeV with the VENUS detector at TRISTAN. Measured R-ratios are consistent with the standard model using the Z-boson mass; 91.1 GeV/c2. Using two new observables, we searched for a planar four-jet and other multi-jet events resulting from the decay of a charge — 1 3 e b quark. Having observed no positive signals, we excluded b masses between 19.4 and 28.2 GeV/c2 with a 95% confidence level, regardless of branching into charged current and loop-induced flavor-changing neutral current decay, including a possible Higgs decay process. The charge + 2 3 e top quark was excluded below f30.2 GeV/c2.
Physics Letters B | 1993
K. Abe; K. Amako; Y. Arai; T. Arima; Y. Asano; M. Chiba; Y. Chiba; M. Daigo; M. Fukawa; Y. Fukushima; J. Haba; Y. Hemmi; M. Higuchi; F. Hinode; T. Hirose; Y. Homma; Y. Hoshi; N. Hosoda; N. Ishihara; E. Kanatani; N. Kanda; Nobuyuki Kanematsu; J. Kanzaki; R. Kikuchi; T. Kondo; T. T. Korhonen; A. E. Krüger; H. Kurashige; J. MacNaughton; T. Matsui
Abstract We have studied c (charm) and b (bottom) quark production at the TRISTAN energy region by tagging prompt electrons from the semileptonic decays. Electrons were identified over a wide momentum range between 1 and 29 GeV/c by a transition-radiation-detector in addition to a lead-glass calorimeter. The production cross sections of c and b quarks and the mean values of the fragmentation functions for c and b quarks were obtained as σc = 55.9±8.8(stat.)±7.9(syst.) pb, σb = 13.1±2.9(stat.)±1.0(syst.) pb, 〈xc〉 = 0.44±0.08(stat.)±0.04(syst.) and 〈xb〉 = 0.72±0.12(stat.)±0.08(syst.), respectively. The forward-backward asymmetries of the c and b quarks were also measured to be −0.57±0.16(stat.)±0.06(syst.) and −0.64±0.26(stat.)± 0.07(syst.), respectively. Both the cross sections and the forward-backward asymmetries of the c and b quarks are consistent with the standard model.
Flow Measurement and Instrumentation | 1990
Nobuyuki Takenaka; Terushige Fujii; K. Akagawa; A. Ono; K. Sonoda; K. Nishizaki; H. Asano
Abstract Visualizations by real-time neutron radiography are demonstrated of various flow patterns of nitrogen gas—water two-phase flow in a stainless-steel tube, water inverted annular flow in a stainless-steel tube, flashing flow in an aluminium nozzle and fluidized bed in aluminium tube and vessels. Photographs every 1/60 s are presented by an image processing method to show the dynamic behaviours of the various flow patterns. It is shown that this visualization method can be applied efficiently to multiphase flow researches and will be applicable to multiphase flows in industrial machines.
Journal of the Physical Society of Japan | 1987
K. Abe; K. Amako; Y. Asano; Herbert Friedrich Boerner; Masami Chiba; Y. Chiba; M. Daigo; T. Emura; I. Endo; M. Fukawa; T. Fukui; Y. Fukushima; J. Haba; I. Hayashibara; Y. Hemmi; M. Higuchi; T. Hirose; Y. Hojyo; Y. Homma; Y. Hoshi; Y. Ikegami; N. Ishihara; T. Kamitani; Nobuyuki Kanematsu; J. Kanzaki; R. Kikuchi; Takahiko Kondo; T. Koseki; K. Kubo; H. Kurashige
A result of the search for the top quark in e + e - annihilation into hadrons at (sqrt{s}=50) GeV is presented. The experiment has been perforrnxed using the VENUS detector at TRISTAN. No evidence has been found for the production of the top quark. From the study using the event shape of the multihadron events, the upper limit of the production cross section is found to be 16 pb at thcc 95% confidence level.
Physics Letters B | 1990
K. Abe; K. Amako; Y. Arai; Y. Asano; Masami Chiba; Y. Chiba; M. Daigo; T. Emura; I. Endo; M. Fukawa; T. Fukui; Y. Fukushima; J. Haba; I. Hayashibara; Y. Hemmi; M. Higuchi; T. Hirose; Y. Hojyo; Y. Homma; Y. Hoshi; Y. Ikegami; N. Ishihara; T. Kamitani; Nobuyuki Kanematsu; J. Kanzaki; R. Kikuchi; T. Kondo; T. Koseki; K. Kubo; H. Kurashige
Abstract We have tested extra Z models in the reactions e+e−→μ+μ−, τ+τ− and hadrons in the energy range 50 s GeV using the VENUS detector at the TRISTAN e+e− storage ring. Our data are in good agreement with the standard model prediction ( χ 2 N Df = 2.9 31 ) ). We have obtained 90% confidence-level lower limits of 105, 125 and 231 GeV for the masses of ZΨ, Zη and Zχ bosons which are expected from the E6 grand unified theory. We also place a 90% confidence-level lower limit of 426 GeV for the mass of an extra-Z boson whose couplings to quarks and leptons are assumed to be the same as those for the standard Z boson. Our results exceed the previous experimental limits from the p p collider experiments, although there have been some combined analyses reporting the limits better than those obtained in the present analysis.
Fusion Engineering and Design | 1995
Nobuyuki Takenaka; Terushige Fujii; A. Ono; Yasunori Motomura; A Turuno
Abstract Experimental techniques were developed to visualize liquid metal flows by neutron radiography. Lead-bismuth eutectic was used as a working fluid. Tracer and dye injection methods were employed for the visualization. A tracer made of gold-cadmium intermetallic compound and a dye made of lead-bismuth-cadmium alloy were developed. It was shown that both methods were suitable for flow visualization in a liquid metal. The use of this visualization technique to study thermal hydraulics in a liquid metal-cooled blanket for a fusion reactor is discussed.
Physics Letters B | 1993
F. Hinode; K. Abe; K. Amako; Y. Arai; T. Arima; Y. Asano; M. Chiba; Y. Chiba; M. Daigo; M. Fukawa; Y. Fukushima; J. Haba; Y. Hemmi; M. Higuchi; T. Hirose; Y. Homma; Y. Hoshi; N. Hosoda; N. Ishihara; N. Kanda; E. Kanatani; Nobuyuki Kanematsu; J. Kanzaki; R. Kikuchi; T. T. Korhonen; T. Kondo; A. E. Krüger; H. Kurashige; J. MacNaughton; T. Matsui
Abstract We have studied the production of charged D ∗ mesons in e + e − annihilation at an average center-of-mass energy of 58.0 GeV. Charged D ∗ mesons were identified using two independent methods; the mass-difference method and the detection of the low transverse-momentum pion. The forward-backward asymmetry of the charm quark production was measured to be A c = −0.61±0.13(stat.)±0.08(syst.). The cross section of inclusive D ∗ production was found to be σ(e + e − →D ∗ ± +X) = 24.5 ± 5.3 ( stat. )±3.0( syst. ) pb. If we assume the standard model prediction for the charm quark production, we obtain the branching ratio for the charm quark to produce a charged D ∗ meson to be Br (c→D ∗+ + X) = (22±5( stat. )±3( syst. ))% .
European Physical Journal C | 1994
S. Uehara; K. Abe; K. Amako; Y. Arai; T. Arima; Y. Asano; M. Chiba; Y. Chiba; Motomasa Daigo; M. Fukawa; Y. Fukushima; J. Haba; H. Hanai; Y. Hemmi; M. Higuchi; F. Hinode; T. Hirose; Y. Homma; N. Hosoda; N. Ishihara; Y. Iwata; N. Kanda; Nobuyuki Kanematsu; J. Kanzaki; R. Kikuchi; T. Kondo; T.T. Korhonen; A. E. Krüger; H. Kurashige; J. MacNaughton
Experimental studies of open charm production in two-photon processes have been performed. In the measurement, charmed hadrons were identified by electrons from their semi-leptonic decays. The result was compared with calculations based on the direct process and photon-gluon fusion process by resolved photons. We found that the effect of the gluon component in a photon is substantial in the observed events.