D. Abe
Tohoku University
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Featured researches published by D. Abe.
Physical Review C | 2004
P. K. Saha; H. Noumi; D. Abe; S. Ajimura; K. Aoki; H. Bhang; K. Dobashi; T. Endo; Y. Fujii; T. Fukuda; Huicheng Guo; O. Hashimoto; H. Hotchi; K. Imai; E. Kim; J.-H. Kim; T. Kishimoto; A. Krutenkova; K. Maeda; T. Nagae; Masato Nakamura; H. Outa; T. Saito; A. Sakaguchi; R. Sawafta; M. Sekimoto; Y. Shimizu; T. Takahashi; H. Tamura; L. Tang
In order to study the Sigma-nucleus optical potential, we measured inclusive (pi^-,K^+) spectra on medium-to-heavy nuclear targets: CH_2, Si, Ni, In and Bi. The CH_2 target was used to calibrate the excitation energy scale by using the elementary process p + pi^- -> K^+ + Sigma^-, where the C spectrum was also extracted. The calibration was done with +-0.1 MeV precision. The angular distribution of the elementary cross section was measured, and agreed well with the previous bubble chamber data, but with better statistics, and the magnitudes of the cross sections of the measured inclusive (pi^-,K^+) spectra were also well calibrated. All of the inclusive spectra were found to be similar in shape at a region near to the Sigma^- binding energy threshold, showing a weak mass-number dependence on the magnitude of the cross section. The measured spectra were compared with a theoretical calculation performed within the framework of the Distorted Wave Impulse Approximation (DWIA). It has been demonstrated that a strongly repulsive \sig-nucleus potential with a non-zero size of the imaginary part is required to reproduce the shape of the measured spectra.
Physical Review C | 2005
A. Krutenkova; V. V. Kulikov; T. Watanabe; D. Abe; Y. Fujii; O. Hashimoto; T. Takahashi; H. Tamura; T. Nagae; H. Noumi; H. Outa; Masato Nakamura
The forward inclusive pion double charge exchange reaction, ^{16}O(pi^-,pi^+)X, at T_0 = 0.50 and 0.75 GeV has been studied in the kinematical region where an additional pion production is forbidden by energy-momentum conservation. The experiment was performed with the SKS spectrometer at KEK PS. The measured ratio of double charge exchange cross-section for these energies dsigma(0.50 GeV)/dOmega / dsigma(0.75 GeV)/dOmega = 1.7 +/- 0.2, disagrees with the value of 7.2 predicted within the conventional sequential single charge exchange mechanism. Possible reasons for the disagreement are discussed in connection with the Glauber inelastic rescatterings.
Physical Review C | 2004
P. K. Saha; Y. Shimizu; M. Sekimoto; A. Sakaguchi; H. Bhang; A. Krutenkova; T. Nagae; T. Watanabe; K. Aoki; H. Outa; D. Abe; Masato Nakamura; L.H. Zhu; S.H. Zhou; E. Kim; S. Ajimura; L. Tang; Huicheng Guo; K. Dobashi; H. Tamura; T. Endo; T. Kishimoto; K. Tanida; T. Saito; H.H. Xia; H. Hotchi; J. H. Kim; H. Noumi; O. Hashimoto; Y. Fujii
In order to study the Sigma-nucleus optical potential, we measured inclusive (pi^-,K^+) spectra on medium-to-heavy nuclear targets: CH_2, Si, Ni, In and Bi. The CH_2 target was used to calibrate the excitation energy scale by using the elementary process p + pi^- -> K^+ + Sigma^-, where the C spectrum was also extracted. The calibration was done with +-0.1 MeV precision. The angular distribution of the elementary cross section was measured, and agreed well with the previous bubble chamber data, but with better statistics, and the magnitudes of the cross sections of the measured inclusive (pi^-,K^+) spectra were also well calibrated. All of the inclusive spectra were found to be similar in shape at a region near to the Sigma^- binding energy threshold, showing a weak mass-number dependence on the magnitude of the cross section. The measured spectra were compared with a theoretical calculation performed within the framework of the Distorted Wave Impulse Approximation (DWIA). It has been demonstrated that a strongly repulsive \sig-nucleus potential with a non-zero size of the imaginary part is required to reproduce the shape of the measured spectra.
Physics of Atomic Nuclei | 2005
A. P. Krutenkova; O. Hashimoto; T. Watanabe; H. Noumi; P. K. Saha; D. Abe; A. B. Kaidalov; V. V. Kulikov; T. Nagae; Masato Nakamura; T. Takahashi; H. Tamura; Y. Fujii
The inclusive cross section for pion double charge exchange on 16O at T0 = 0.5 and 0.75 GeV was measured with the superconducting kaon spectrometer (SKS) at KEK in a joint ITEP/KEK experiment. The result shows a relatively weak energy dependence of the measured cross section, which is in contradiction with its rapid drop predicted within the conventional model of two sequential single charge exchanges. The data of this experiment agree with the results that were obtained previously from similar measurements at ITEP and which are indicative of a significant contribution from the mechanism of inelastic Glauber rescatterings for T0 ≳ 0.6 GeV.
Physical Review C | 2005
A. Krutenkova; T. Watanabe; D. Abe; Y. Fujii; O. Hashimoto; V. V. Kulikov; T. Nagae; Masato Nakamura; H. Noumi; H. Outa; P. K. Saha; T. Takahashi; H. Tamura
The forward inclusive pion double charge exchange reaction, ^{16}O(pi^-,pi^+)X, at T_0 = 0.50 and 0.75 GeV has been studied in the kinematical region where an additional pion production is forbidden by energy-momentum conservation. The experiment was performed with the SKS spectrometer at KEK PS. The measured ratio of double charge exchange cross-section for these energies dsigma(0.50 GeV)/dOmega / dsigma(0.75 GeV)/dOmega = 1.7 +/- 0.2, disagrees with the value of 7.2 predicted within the conventional sequential single charge exchange mechanism. Possible reasons for the disagreement are discussed in connection with the Glauber inelastic rescatterings.
Physical Review C | 2005
A. Krutenkova; T. Watanabe; D. Abe; Y. Fujii; O. Hashimoto; V. V. Kulikov; T. Nagae; Masato Nakamura; H. Noumi; H. Outa; P. K. Saha; T. Takahashi; H. Tamura
The forward inclusive pion double charge exchange reaction, ^{16}O(pi^-,pi^+)X, at T_0 = 0.50 and 0.75 GeV has been studied in the kinematical region where an additional pion production is forbidden by energy-momentum conservation. The experiment was performed with the SKS spectrometer at KEK PS. The measured ratio of double charge exchange cross-section for these energies dsigma(0.50 GeV)/dOmega / dsigma(0.75 GeV)/dOmega = 1.7 +/- 0.2, disagrees with the value of 7.2 predicted within the conventional sequential single charge exchange mechanism. Possible reasons for the disagreement are discussed in connection with the Glauber inelastic rescatterings.
Physical Review C | 2004
P. K. Saha; H. Noumi; K. Aoki; T. Fukuda; T. Nagae; H. Outa; M. Sekimoto; D. Abe; K. Dobashi; T. Endo; Y. Fujii; O. Hashimoto; K. Maeda; T. Takahashi; H. Tamura; T. Watanabe; S. Ajimura; T. Kishimoto; A. Sakaguchi
In order to study the Sigma-nucleus optical potential, we measured inclusive (pi^-,K^+) spectra on medium-to-heavy nuclear targets: CH_2, Si, Ni, In and Bi. The CH_2 target was used to calibrate the excitation energy scale by using the elementary process p + pi^- -> K^+ + Sigma^-, where the C spectrum was also extracted. The calibration was done with +-0.1 MeV precision. The angular distribution of the elementary cross section was measured, and agreed well with the previous bubble chamber data, but with better statistics, and the magnitudes of the cross sections of the measured inclusive (pi^-,K^+) spectra were also well calibrated. All of the inclusive spectra were found to be similar in shape at a region near to the Sigma^- binding energy threshold, showing a weak mass-number dependence on the magnitude of the cross section. The measured spectra were compared with a theoretical calculation performed within the framework of the Distorted Wave Impulse Approximation (DWIA). It has been demonstrated that a strongly repulsive \sig-nucleus potential with a non-zero size of the imaginary part is required to reproduce the shape of the measured spectra.
Archive | 2000
H. Tamura; D. Abe; S. Ajimura; H. Akikawa; K. Araki; H. Bhang; R. E. Chrien; T. Endo; P. Eugenio; G. B. Franklin; Y. Fujii; T. Fukuda; L. Gan; O. Hashimoto; H. Hotchi; K. Imai; Y. Kakiguchi; P. Khaustov; J. H. Kim; Y. D. Kim; H. Kohri; M. May; T. Miyoshi; T. Murakami; T. Nagae; J. Nakano; H. Noumi; H. Outa; K. Ozawa; P. Pile
We report on the first two experiments of hypernuclear γ-ray spectroscopy with Hyperball, a large-acceptance germanium detector system. In a KEK experiment, we observed two γ transitions in Λ 7 Li, the spin- flip M1(3/2+ → 1/2+) at 691.7 ± 0.6 stat ± 1.0 sys keV and the E2(5/2+ → 1/2+) at 2050.4 ± 0.4 stat ± 0.7 sys keV. The former gives unambiguous information on the strength of the ΛN spin-spin interaction. B(E2) of the latter transition was measured to be \( 3.6 \pm {0.5^{stat}}\,_{ - 0.4}^{ + 0.5}{\,^{sys}}{e^2}f{m^4} \). In the second experiment at BNL, we observed the E2(5/2+, 3/2+ → 1/2+) transitions of Λ 9 Be at around 3.05 MeV.
Physical Review Letters | 2000
H. Tamura; K. Tanida; D. Abe; H. Akikawa; Kiyomichi Araki; H. Bhang; T. Endo; Y. Fujii; T. Fukuda; O. Hashimoto; K. Imai; H. Hotchi; Y. Kakiguchi; J.-H. Kim; Y. D. Kim; T. Miyoshi; T. Murakami; T. Nagae; H. Noumi; H. Outa; K. Ozawa; T. Saito; J. Sasao; S. Satoh; R. Sawafta; M. Sekimoto; T. Takahashi; L. Tang; H.H. Xia; S.H. Zhou
Physical Review Letters | 2001
K. Tanida; H. Tamura; D. Abe; H. Akikawa; Kiyomichi Araki; H. Bhang; T. Endo; Y. Fujii; T. Fukuda; O. Hashimoto; K. Imai; H. Hotchi; Y. Kakiguchi; J.-H. Kim; Y. D. Kim; T. Miyoshi; T. Murakami; T. Nagae; H. Noumi; H. Outa; K. Ozawa; T. Saito; J. Sasao; S. Satoh; R. Sawafta; M. Sekimoto; T. Takahashi; L. Tang; H.H. Xia; S.H. Zhou