NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.Iseri Found 39 matches. 2021IS06 Phys.Rev. C 103, 044605 (2021) Prediction of the analyzing power for p(pol) + 6He elastic scattering at 200 MeV from p(pol) + 4He elastic scattering at 200 MeV NUCLEAR REACTIONS 4,6He(polarized p, p), E=71, 72, 200 MeV; analyzed experimental data for differential σ(E, θ), Ay(E, θ) and form factor F(Q) versus Q using improved valence-target-cutting (VTC) theory and cluster-folding (CF) model.
doi: 10.1103/PhysRevC.103.044605
2011OG12 J.Phys.:Conf.Ser. 312, 082008 (2011) K.Ogata, T.Matsumoto, S.Hashimoto, K.Minomo, T.Egami, Y.Iseri, M.Kohno, S.Chiba, C.A.Bertulani, Y.R.Shimizu, M.Kamimura, M.Yahiro Status of breakup reaction theory NUCLEAR REACTIONS 7Li(d, γ), (d, n), (d, p), E=10-50 MeV; calculated σ. 90Zr(p, p), E=65, 800 MeV; calculated dσ with and without Brieva-Rook localization. 208Pb(8B, X), E=250 MeV/nucleon; calculated breakup σ including relativistic corrections. 209Bi(6He, 6He), E=22.5 MeV; calculated σ with and without breakup effects, B(E1) strength distribution. Three- and four-body CDCC.
doi: 10.1088/1742-6596/312/4/082008
2011SA39 Phys.Rev. C 84, 024604 (2011) S.Sakaguchi, Y.Iseri, T.Uesaka, M.Tanifuji, K.Amos, N.Aoi, Y.Hashimoto, E.Hiyama, M.Ichikawa, Y.Ichikawa, S.Ishikawa, K.Itoh, M.Itoh, H.Iwasaki, S.Karataglidis, T.Kawabata, T.Kawahara, H.Kuboki, Y.Maeda, R.Matsuo, T.Nakao, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, A.Tamii, T.Wakui, K.Yako, M.Yamaguchi, Y.Yamamoto Analyzing power in elastic scattering of 6He from a polarized proton target at 71 MeV/nucleon NUCLEAR REACTIONS 1H(6He, 6He), [6He secondary beam from 9Be(12C, X), E=92 MeV/nucleon primary reaction], E=71 MeV/nucleon; measured 6He and proton spectra, (6He)(p)(q, φ), p(θ), vector analyzing powers, polarized target, σ(θ); deduced optical model parameters. Comparison with semimicroscopic analysis with an α+n+n cluster folding model.
doi: 10.1103/PhysRevC.84.024604
2010UE01 Phys.Rev. C 82, 021602 (2010) T.Uesaka, S.Sakaguchi, Y.Iseri, K.Amos, N.Aoi, Y.Hashimoto, E.Hiyama, M.Ichikawa, Y.Ichikawa, S.Ishikawa, K.Itoh, M.Itoh, H.Iwasaki, S.Karataglidis, T.Kawabata, T.Kawahara, H.Kuboki, Y.Maeda, R.Matsuo, T.Nakao, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, M.Tanifuji, A.Tamii, T.Wakui, K.Yako, Y.Yamamoto, M.Yamaguchi Analyzing power for proton elastic scattering from the neutron-rich 6He nucleus NUCLEAR REACTIONS 1H(6He, 6He), E=71 MeV/nucleon; measured σ(θ), vector analyzing power, polarized proton solid target. Comparison with t-matrix and g-matrix microscopic folding calculations. Discussed α-core distribution in 6He.
doi: 10.1103/PhysRevC.82.021602
2009OG04 J.Phys.Soc.Jpn. 78, 084201 (2009) K.Ogata, T.Matsumoto, Y.Iseri, M.Yahiro Properties of Nuclear and Coulomb Breakup of 8B NUCLEAR REACTIONS 12C, 16O, 40Ca, 58Ni, 90Zr, 152Sm, 208Pb(8B, p7Be), E=65 MeV/nucleon; calculated dependence of breakup σ on target mass; deduced nuclear-Coulomb interference. Continuum-discretized coupled-channels (CDCC) method.
doi: 10.1143/JPSJ.78.084201
2008OG01 Nucl.Phys. A805, 447c (2008) K.Ogata, T.Matsumoto, T.Egami, Y.Iseri, M.Kamimura, M.Yahiro Full coupled-channel description of three-body and four-body breakup reactions NUCLEAR REACTIONS 208Pb(8B, X), E=52 MeV/nucleon; calculated breakup σ(θ) with eikonal CDCC; deduced 7Be(p, γ) astrophysical S-factor. 209Bi(6He, 6He), E=19, 22.5 MeV; calculated total, elastic σ(θ) using four-body CDCC. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.02.283
2006MA31 Phys.Rev. C 73, 051602 (2006) T.Matsumoto, T.Egami, K.Ogata, Y.Iseri, M.Kamimura, M.Yahiro Coulomb breakup effects on the elastic cross section of 6He + 209Bi scattering near Coulomb barrier energies NUCLEAR REACTIONS 209Bi(6He, 6He), E=19, 22.5 MeV; analyzed elastic σ(θ), Coulomb breakup effects. Four-body continuum-discretized coupled-channels model.
doi: 10.1103/PhysRevC.73.051602
2006OG01 Phys.Rev. C 73, 024605 (2006) K.Ogata, S.Hashimoto, Y.Iseri, M.Kamimura, M.Yahiro Determination of S17 from 8B breakup by means of the method of continuum-discretized coupled channels NUCLEAR REACTIONS 208Pb(8B, p7Be), E=52 MeV/nucleon; analyzed σ(θ). 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled channels method.
doi: 10.1103/PhysRevC.73.024605
2005IS08 Phys.Rev. C 72, 027601 (2005); Erratum Phys.Rev. C 72, 039901 (2005) S.Ishikawa, M.Tanifuji, Y.Iseri, Y.Yamamoto Relationships among depolarizations in scattering of polarized protons from 3He at intermediate energies NUCLEAR REACTIONS 3He(polarized p, p), E=800 MeV; calculated depolarization observables, spin-spin and spin-independent interaction contributions.
doi: 10.1103/PhysRevC.72.027601
2005TA34 Eur.Phys.J. A 25, Supplement 1, 273 (2005) M.Takashina, Y.Sakuragi, Y.Iseri Effect of halo structure on 11Be + 12C elastic scattering NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ). Continuum-discretized coupled-channels method, comparison with data.
doi: 10.1140/epjad/i2005-06-077-1
2004EG04 Phys.Rev. C 70, 047604 (2004) T.Egami, K.Ogata, T.Matsumoto, Y.Iseri, M.Kamimura, M.Yahiro Gaussian expansion approach to nuclear and Coulomb breakup NUCLEAR REACTIONS 58Ni(8B, p7Be), E=25.8 MeV; calculated breakup σ(θ), Coulomb and nuclear contributions. Continuum discretized coupled channels approach, comparison with data.
doi: 10.1103/PhysRevC.70.047604
2004IS04 Phys.Rev. C 69, 034001 (2004) S.Ishikawa, M.Tanifuji, Y.Iseri, Y.Yamamoto Polarization phenomena in hyperon-nucleon scattering
doi: 10.1103/PhysRevC.69.034001
2004MA57 Nucl.Phys. A738, 471 (2004) T.Matsumoto, E.Hiyama, M.Yahiro, K.Ogata, Y.Iseri, M.Kamimura Four-body CDCC analysis of 6He + 12C scattering NUCLEAR REACTIONS 12C(6He, 6He), E=38.3 MeV/nucleon; analyzed σ(θ); deduced halo effects. Continuum-discretized coupled-channels approach.
doi: 10.1016/j.nuclphysa.2004.04.089
2004MB01 Phys.Rev. C 70, 061601 (2004) T.Matsumoto, E.Hiyama, K.Ogata, Y.Iseri, M.Kamimura, S.Chiba, M.Yahiro Continuum-discretized coupled-channels method for four-body nuclear breakup in 6He+12C scattering NUCLEAR REACTIONS 12C(6He, 6He), (6He, 2nα), E=18, 229.8 MeV; calculated elastic and breakup σ(θ), reaction σ. Continuum-discretized coupled-channels method, comparison with data.
doi: 10.1103/PhysRevC.70.061601
2004OG09 Nucl.Phys. A738, 421 (2004) K.Ogata, M.Yahiro, Y.Iseri, T.Matsumoto, N.Yamashita, T.Kamizato, M.Kamimura Determination of S17 from 8B Coulomb dissociation NUCLEAR REACTIONS 58Ni(8B, p7Be), E=25.8 MeV; analyzed σ(θ); deduced asymptotic normalization coefficient. 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled-channels approach.
doi: 10.1016/j.nuclphysa.2004.04.078
2003IS05 Phys.Rev. C 67, 061001 (2003) S.Ishikawa, M.Tanifuji, Y.Iseri Central and tensor components of three-nucleon forces in low-energy proton-deuteron scattering NUCLEAR REACTIONS 2H(p, p), E=0.5-3.0 MeV; calculated σ(θ), vector and tensor analyzing powers; deduced three-nucleon force contributions. Comparison with data.
doi: 10.1103/PhysRevC.67.061001
2003MA91 Phys.Rev. C 68, 064607 (2003) T.Matsumoto, T.Kamizato, K.Ogata, Y.Iseri, E.Hiyama, M.Kamimura, M.Yahiro New treatment of breakup continuum in the method of continuum discretized coupled channels NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; 40Ca(6Li, 6Li), (6Li, X), E=156 MeV; calculated elastic σ, breakup S-matrix elements. Continuum discretized coupled channels, pseudostate discretization.
doi: 10.1103/PhysRevC.68.064607
2003OG02 Phys.Rev. C 67, 011602 (2003); Erratum Phys.Rev. C 67, 019902 (2003) K.Ogata, M.Yahiro, Y.Iseri, M.Kamimura Determination of S17 from the 7Be(d, n)8B reaction NUCLEAR REACTIONS 7Li(d, d), E=8 MeV; 7Li(n, n), E=4.26 MeV; 7Be(d, n), E=7.5 MeV; analyzed σ(θ); deduced parameters. 7Be(p, γ), E not given; deduced astrophysical S-factor. Continuum-discretized coupled channels, three-body model.
doi: 10.1103/PhysRevC.67.011602
2003OG06 Phys.Rev. C 68, 064609 (2003) K.Ogata, M.Yahiro, Y.Iseri, T.Matsumoto, M.Kamimura New coupled-channel approach to nuclear and Coulomb breakup reactions NUCLEAR REACTIONS 58Ni(8B, p7Be), E=240 MeV; calculated breakup σ(θ). Hybrid calculation.
doi: 10.1103/PhysRevC.68.064609
2003TA04 Phys.Rev. C 67, 037601 (2003) M.Takashina, S.Takagi, Y.Sakuragi, Y.Iseri Continuum-discretized coupled-channels study of the 11Be → 10Be+n breakup effect on 11Be elastic scattering NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), contribution of projectile breakup effect; deduced dynamical polarization potential. Continuum-discretized coupled-channels approach, comparison with data.
doi: 10.1103/PhysRevC.67.037601
2002IS10 Phys.Rev. C66, 044005 (2002) S.Ishikawa, M.Tanifuji, Y.Iseri Spin observables in nucleon-deuteron scattering and three-nucleon forces NUCLEAR REACTIONS 2H(n, n), (p, p), E=3 MeV; calculated scattering amplitudes, Ay(θ), other polarization observables; deduced three-nucleon force effects.
doi: 10.1103/PhysRevC.66.044005
2002TA31 Prog.Theor.Phys.(Kyoto), Suppl. 146, 630 (2002) S.Takagi, M.Takashina, Y.Sakuragi, Y.Iseri A CDCC Study of 11Be → 10Be + n Breakup Effect on the 11Be Elastic Scattering NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), breakup channel contribution. Continuum-discretized coupled-channels method, comparison with data.
doi: 10.1143/PTPS.146.630
2001IS06 Phys.Rev. C64, 024001 (2001) S.Ishikawa, M.Tanifuji, Y.Iseri Complete Set of Total Cross Sections for Imaginary Parts of nd Forward Scattering Amplitudes, and Three-Nucleon Force Effects NUCLEAR REACTIONS 2H(n, n), E=2-15 MeV; calculated total σ, forward scattering ampltudes; deduced three-nucleon force effects.
doi: 10.1103/PhysRevC.64.024001
2000TA01 Phys.Rev. C61, 024602 (2000) M.Tanifuji, S.Ishikawa, Y.Iseri, T.Uesaka, N.Sakamoto, Y.Satou, K.Itoh, H.Sakai, A.Tamii, T.Ohnishi, K.Sekiguchi, K.Yako, S.Sakoda, H.Okamura, K.Suda, T.Wakasa Reaction Mechanism and Characteristics of T20 in d + 3He Backward Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 3He(polarized d, d), E=140, 200, 270 MeV; measured backward scattering σ(θ), T20. 3He(polarized d, d), (polarized d, X), E at < 3 GeV/c; calculated T20, spin observables; deduced proton transfer contribution, other reaction mechanism features. PWIA analysis.
doi: 10.1103/PhysRevC.61.024602
1998TA08 Phys.Rev. C57, 2493 (1998) M.Tanifuji, S.Ishikawa, Y.Iseri New Approach to Polarization Phenomena in dp Backward Elastic Scattering at Intermediate and High Energies NUCLEAR REACTIONS 2H(polarized p, p), E not given; calculated backscattering T20, other spin observables; deduced imaginary amplitudes role.
doi: 10.1103/PhysRevC.57.2493
1998TA10 Nucl.Instrum.Methods Phys.Res. A402, 433 (1998) M.Tanifuji, S.Ishikawa, Y.Iseri Forward Polarization Observables in 3He(d, p)4He Reactions NUCLEAR REACTIONS 3He(polarized d, p), E not given; calculated T20, polarization transfer coefficients.
doi: 10.1016/S0168-9002(97)00886-3
1995IS05 Phys.Lett. 354B, 183 (1995) Virtual Breakup to Spin-Singlet States in Elastic Scattering of Deuterons from Nuclei NUCLEAR REACTIONS 58Ni(polarized d, d), E=80, 400 MeV; analyzed σ(θ), analyzing power vs θ; deduced deuteron virtual breakup contribution. Coupled-discretized continuum channels approach.
doi: 10.1016/0370-2693(95)00679-F
1991IS06 Nucl.Phys. A533, 574 (1991) Y.Iseri, M.Tanifuji, H.Kameyama, M.Kamimura, M.Yahiro Spin-Dependent Interactions and Polarization Observables in Elastic Scattering of Deuterons at Intermediate Energies NUCLEAR REACTIONS 58Ni(polarized d, d), E=700 MeV; calculated vector, tensor analyzing power vs θ.
doi: 10.1016/0375-9474(91)90534-D
1991IS07 Phys.Lett. 265B, 207 (1991) Y.Iseri, M.Tanifuji, Y.Aoki, M.Kawai Effects of Tensor Interaction in p-n Breakup States on Deuteron Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized d, d), E=56 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ; deduced tensor interaction role in p-n breakup.
doi: 10.1016/0370-2693(91)90042-O
1989LU03 Prog.Theor.Phys.(Kyoto) 81, 396 (1989) Bare Potential DWBR in Rearrangement Reactions NUCLEAR REACTIONS 40Ca(d, p), E=10.5, 26.7 MeV; 16O(d, p), E=10.5, 24.89 MeV; calculated σ(θ). Bare potential DWBA.
doi: 10.1143/PTP.81.396
1989TA07 Phys.Lett. 217B, 375 (1989) M.Tanifuji, H.Kameyama, M.Kamimura, Y.Iseri, M.Yahiro T(R) and T(L) Tensor Interactions in Deuteron Elastic Scattering NUCLEAR REACTIONS 58Ni(polarized d, d), E=700 MeV; calculated σ(θ), analyzing power.
doi: 10.1016/0370-2693(89)90063-4
1988IS02 Nucl.Phys. A490, 383 (1988) Y.Iseri, H.Kameyama, M.Kamimura, M.Yahiro, M.Tanifuji Virtual Breakup Effects in Elastic Scattering of Polarized Deuterons NUCLEAR REACTIONS 16O, 40Ca, 58Ni, 118Sn, 208Pb(polarized d, d), E=56 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ; deduced reaction mechansim.
doi: 10.1016/0375-9474(88)90512-X
1987YA06 Nucl.Phys. A463, 435c (1987) M.Yahiro, Y.Iseri, H.Kameyama, M.Kamimura, M.Kawai, M.Tanifuji Deuteron Breakup Effects on Deuteron Elastic Scattering NUCLEAR REACTIONS 58Ni, 208Pb(polarized d, d), E=56, 400 MeV; calculated σ(θ), analyzing powers; deduced deuteron breakup effects. Coupled discretized continuum channels method.
doi: 10.1016/0375-9474(87)90687-7
1986IS04 Phys.Rev. C34, 38 (1986) Anomalous Absorption of Proton Partial Waves by the Optical Potential NUCLEAR REACTIONS 10B, 52Cr, 142Ce(p, p), E(cm)=3.454-15.382 MeV; 24Mg, 85Rb, 209Bi(p, p), E(cm)=6.802-20.227 MeV; 4He, 28Si, 87Rb, 208Pb(p, p), E(cm)=6.719-20.848 MeV; 40Ar, 132,128Xe, 9Be, 48Ti(p, p), E(cm)=10.964-17.16 MeV; 16O, 65Cu, 176Lu(p, p), E(cm)=15.741-21.412 MeV; 21Ne, 74Ge, 191Ir(p, p), E(cm)=17.063-22.559 MeV; 25Mg, 96Mo, 232Th(p, p), E(cm)=22.099-26.232 MeV; 40Ca, 113In, 238U(p, p), E(cm)=21.31-28.522 MeV; 40K, 126Te(p, p), E(cm)=27.012, 25.351 MeV; 56Fe, 156Dy(p, p), E(cm)=27.254-27.28 MeV; 57Fe, 170Yb(p, p), E(cm)=32.253, 30.607 MeV; 79Br, 196Pt(p, p), E(cm)=32.254, 32.221 MeV; 80Kr, 208Pb(p, p), E(cm)=37.105, 35.723 MeV; 110Cd, 238U(p, p), E(cm)=36.98, 38.367 MeV; 105Pd(p, p), E(cm)=42.414 MeV; 140Ce(p, p), E(cm)=41.958 MeV; 130Xe(p, p), E(cm)=47.862 MeV; 180Ta(p, p), E(cm)=46.818 MeV; 160Gd(p, p), E(cm)=53.181 MeV; 232Th(p, p), E(cm)=50.451 MeV; 193Ir(p, p), E(cm)=59.707 MeV; 209Bi(p, p), E(cm)=69.893 MeV; 238U(p, p), E(cm)=76.808 MeV; analyzed data; deduced anomalous absorption.
doi: 10.1103/PhysRevC.34.38
1986YA11 Phys.Lett. 182B, 135 (1986) M.Yahiro, H.Kameyama, Y.Iseri, M.Kamimura, M.Kawai Coupled-Channel Approach to Deuteron Elastic Scattering at Intermediate Energy NUCLEAR REACTIONS 40Ca(polarized p, p), E=200 MeV; analyzed σ(θ), analyzing power vs θ; deduced proton optical potentials; 58Ni(polarized d, d), E=400 MeV; calculated σ(θ), vector, tensor analyzing powers. Coupled channels method.
doi: 10.1016/0370-2693(86)91563-7
1985KA01 Phys.Rev. C31, 400 (1985) Anomalous Absorption of Neutron Partial Waves by the Nuclear Optical Potential NUCLEAR STRUCTURE A=9-232; analyzed anomalous neutron partial wave strong absorption; deduced systematics. Optical model fits input.
doi: 10.1103/PhysRevC.31.400
1984YA01 Phys.Lett. 141B, 19 (1984) M.Yahiro, Y.Iseri, M.Kamimura, M.Nakano A Coupled-Channel Approach to Deuteron Projectile Breakup NUCLEAR REACTIONS 12C, 51V, 118Sn(d, np), E=56 MeV; calculated σ(θn, θp, Ep), σ(breakup). Three-body model, discretized continuum coupled channels.
doi: 10.1016/0370-2693(84)90549-5
1983IS06 Prog.Theor.Phys.(Kyoto) 69, 1038 (1983) Investigation of Adiabatic Approximation of Deuteron-Breakup Effect on (d, p) Reactions NUCLEAR REACTIONS 58Ni(d, d), (d, p), E=80 MeV; analyzed σ(θ); deduced adiabatic approximation limitation, breakup wave function role.
doi: 10.1143/PTP.69.1038
1982YA03 Prog.Theor.Phys.(Kyoto) 67, 1467 (1982) M.Yahiro, M.Nakano, Y.Iseri, M.Kamimura Coupled-Discretized-Continuum-Channels Method for Deuteron Breakup Reactions Based on Three-Body Model - Justification of the Method for Truncation and Discretization of the p-n Continuum - NUCLEAR REACTIONS, ICPND 58Ni(d, d), (d, np), E=80 MeV; calculated σ(elastic), breakup σ. Coupled-channels method, continuum discretization.
doi: 10.1143/PTP.67.1467
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