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NSR database version of May 24, 2024.

Search: Author = Y.Iseri

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2021IS06      Phys.Rev. C 103, 044605 (2021)

M.Ishii, Y.Iseri, M.Yahiro

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2287.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2287.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1722.


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
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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
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1995IS05      Phys.Lett. 354B, 183 (1995)

Y.Iseri, M.Tanifuji

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
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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
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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
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1989LU03      Prog.Theor.Phys.(Kyoto) 81, 396 (1989)

Y.L.Luo, Y.Iseri, M.Kawai

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
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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
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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
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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
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1986IS04      Phys.Rev. C34, 38 (1986)

Y.Iseri, M.Kawai

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
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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
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1985KA01      Phys.Rev. C31, 400 (1985)

M.Kawai, Y.Iseri

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
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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
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1983IS06      Prog.Theor.Phys.(Kyoto) 69, 1038 (1983)

Y.Iseri, M.Yahiro, M.Nakano

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
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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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