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NSR database version of April 11, 2024.

Search: Author = H.Horie

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1988YO03      Phys.Rev. C38, 1058 (1988)

A.Yokoyama, H.Horie

Shell-Model Calculations of Isovector Electromagnetic Transitions and Gamow-Teller Beta Decays in the N ≈ 28 Region

NUCLEAR STRUCTURE ⁴⁹Ca, ^49,50Sc, ^50,51Ti, ^51,52V, ^52,53Cr, ⁵³Mn, ⁵⁵Fe, ⁵⁵Co; calculated magnetic dipole moments, isovector E2, M1 transition strength, isobaric analog states, Gamow-Teller beta decay log ft values. Shell model.

doi: 10.1103/PhysRevC.38.1058
Citations: PlumX Metrics

1987YO04      Phys.Rev. C36, 1657 (1987)

A.Yokoyama, H.Horie

Core-Polarization Effects on Stretched Particle-Hole Excitations in Closed Shell Nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ²⁸Si, ^48,40Ca, ⁹⁰Zr, ¹⁴⁶Gd, ²⁰⁸Pb; calculated stretched particle-hole excitation suppression factors. Configuration mixing model.

doi: 10.1103/PhysRevC.36.1657
Citations: PlumX Metrics

1985MU06      Nucl.Phys. A440, 254 (1985)

K.Muto, H.Horie

Shell-Model Study on Magnetic Dipole Excitation of N = 28 Isotopes

NUCLEAR REACTIONS ⁵¹V(p, p'), E=200 MeV; ⁵¹V(e, e'), E=38, 49, 57 MeV; calculated σ(Ep'), σ(E(e')).

NUCLEAR STRUCTURE ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe, ⁵¹V; calculated B(M1) strength distribution, g.

doi: 10.1016/0375-9474(85)90340-9
Citations: PlumX Metrics

1985MU23      Phys.Lett. 165B, 25 (1985)

K.Muto, H.Yamazaki, T.Oda, H.Horie

Shell-Model Study on Gamow-Teller Excitation of ⁹⁰Zr

NUCLEAR REACTIONS ⁹⁰Zr(p, n), E=120 MeV; calculated Gamow-Teller transition strength distribution. Shell model.

doi: 10.1016/0370-2693(85)90683-5
Citations: PlumX Metrics

1985YO01      Phys.Rev. C31, 1012 (1985)

A.Yokoyama, H.Horie

Intruder States of the Odd-Mass N = 27 Isotones

NUCLEAR STRUCTURE ⁴⁷Ca, ^48,49Sc, ^49,50Ti, ^53,54Fe, ⁵¹V, ⁵²Cr, ⁵³Mn, ⁵⁵Co; calculated levels. ⁴⁷Ca, ⁴⁹Ti, ⁵¹Cr, ⁵³Fe; calculated B(E2). Shell model, effective interactions.

doi: 10.1103/PhysRevC.31.1012
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1984MU03      Phys.Lett. 135B, 349 (1984)

K.Muto, T.Shimano, H.Horie

Neutron Core-Excited High-Spin States in N = 50 Nuclei

NUCLEAR STRUCTURE ⁹⁴Rb, ⁹¹Nb; calculated high-spin levels. Shell model.

doi: 10.1016/0370-2693(84)90291-0
Citations: PlumX Metrics

1984MU09      Phys.Lett. 138B, 9 (1984)

K.Muto, H.Horie

Shell-Model Study on M1 Strength Distributions in N = 28 Isotones

NUCLEAR STRUCTURE ⁴⁸Ca, ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe; analyzed electron, proton inelastic scattering data; deduced B(M1) vs excitation, reduction factor. Shell model.

doi: 10.1016/0370-2693(84)91861-6
Citations: PlumX Metrics

1984TS05      Phys.Lett. 143B, 293 (1984)

T.Tsuboi, K.Muto, H.Horie

Double Beta Decay Nuclear Matrix Element of ⁴⁸Ca

RADIOACTIVITY ⁴⁸Ca(2β); calculated T_1/2, nuclear matrix elements, average β-decay energies, lepton conserving mode. Shell model.

doi: 10.1016/0370-2693(84)91468-0
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1983MU14      Phys.Lett. 127B, 291 (1983)

K.Muto, H.Horie

Monte Carlo Calculation of Gamow-Teller Transition Strength Function

NUCLEAR STRUCTURE ²⁰⁸Bi; calculated Gamow-Teller resonances, Γ, transition strength distribution; deduced particle, hole spreading interference effects. Monte Carlo calculation.

doi: 10.1016/0370-2693(83)91002-X
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1982IW01      Phys.Rev. C25, 658 (1982)

T.Iwamoto, H.Horie, A.Yokoyama

Inelastic Electron Scattering Form Factors for the Excitation of the 2⁺ States in the 1f_7/2 Nuclei

NUCLEAR REACTIONS ^42,44,46,48Ca, ^46,48,50Ti, ^50,52Cr, ⁵⁴Fe(e, e'), E not given; calculated form factors. Shell model, effective interactions.

NUCLEAR STRUCTURE ^42,44,46,48Ca, ^46,48,50Ti, ^50,52Cr, ⁵⁴Fe; calculated levels, B(E2), quadrupole moment. Shell model, effective interactions.

doi: 10.1103/PhysRevC.25.658
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1982MU16      Phys.Lett. 118B, 261 (1982)

K.Muto, T.Oda, H.Horie

Shell-Model Study of the Gamow-Teller Giant Resonance in ²⁰⁸Bi

NUCLEAR STRUCTURE ²⁰⁸Bi; calculated Gamow-Teller resonance fragmentation, transition strength distribution. Shell model.

doi: 10.1016/0370-2693(82)90180-0
Citations: PlumX Metrics

1981YO01      Phys.Lett. 99B, 5 (1981)

A.Yokoyama, T.Oda, H.Horie

Effect of Neutron Excitations on the Strength Distributions for Single-Proton Transfer Reactions on the N=28 Nuclei

NUCLEAR REACTIONS ⁵¹V(³He, d), E=10.48, 15, 22 MeV; analyzed spectroscopic factor data; deduced neutron excitation effects on proton 2p_3/2 strength fragmentation. Shell model.

doi: 10.1016/0370-2693(81)90792-9
Citations: PlumX Metrics

1980HO14      Prog.Theor.Phys.(Kyoto) 63, 872 (1980)

T.Honda, Y.Kudo, H.Horie

A Study of Five-Nucleon Transfer Mechanisms in the (p, ⁶Li) Reactions

NUCLEAR REACTIONS ¹⁶O, ¹¹B(p, ⁶Li), E=51.9 MeV; analyzed σ(θ). Finite-range DWBA, cluster coupling shell model spectroscopic factors.

doi: 10.1143/PTP.63.872
Citations: PlumX Metrics

1978KU02      Progr.Theor.Phys. 59, 101 (1978)

Y.Kudo, T.Honda, H.Horie

Multi-Nucleon Transfer Reaction and Nuclear Spectroscopy

NUCLEAR REACTIONS ¹²C(p, ⁶Li), E=51.9 MeV; calculated σ(θ). DWBA calculations.

doi: 10.1143/PTP.59.101
Citations: PlumX Metrics

1978MU17      Prog.Theor.Phys. 60, 1350 (1978)

K.Muto, T.Oda, H.Horie

A Shell-Model Study of f₇/₂-Shell Nuclei in the Pure f(n)₇/₂ Configuration

NUCLEAR STRUCTURE ^41,42,43Ca, ^{41,43,44,45,46,47}Sc, ^45,47,49Ti, ^48,49,50,51V, ^49,51Cr, ^51,52,53Mn, ⁵⁴Fe, ⁵⁵Co; calculated energy levels, electromagnetic properties, β-decay. Pure f7/2 shell model, effective interaction.

doi: 10.1143/PTP.60.1350
Citations: PlumX Metrics

1978YO04      Prog.Theor.Phys. 60, 427 (1978)

A.Yokoyama, T.Oda, H.Horie

Shell-Model Study of the N - 28 Nuclei with Emphasis on High-Spin States

NUCLEAR STRUCTURE ⁴⁹Sc, ⁵¹V, ⁵³Mn, ⁵⁵Co; calculated energies of high spin states. Shell-model calculation in (f7/2)(f7/2p3/2) space, effective interactions.

doi: 10.1143/PTP.60.427
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1973HO44      Nucl.Phys. A216, 407 (1973)

H.Horie, K.Ogawa

Proton-Neutron Correlations in Nuclei with N = 30

NUCLEAR STRUCTURE ⁵⁰Ca, ⁵¹Sc, ⁵²Ti, ⁵³V, ⁵⁴Cr, ⁵⁵Mn, ⁵⁶Fe, ⁵⁷Co, ⁵⁸Ni; calculated levels, J, π, γ-branching, T_1/2, μ, quadrupole moment, S, B(E2).

doi: 10.1016/0375-9474(73)90476-4
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1971AR27      Nucl.Phys. A173, 97 (1971)

K.Arita, H.Horie

The Non-Normal Parity States of ²⁰⁹Bi and ²⁰⁷Pb

NUCLEAR STRUCTURE ²⁰⁹Bi, ²⁰⁷Pb; calculated non-normal parity levels. Shell model; 1h-2p, 2h-1p configurations.

doi: 10.1016/0375-9474(71)90750-0
Citations: PlumX Metrics

1971HO33      Progr.Theor.Phys. 46, 439 (1971)

H.Horie, K.Ogawa

Effective Proton-Neutron Interaction and Spectroscopy of the Nuclei with N = 29

NUCLEAR STRUCTURE ⁵¹Ti, ⁵³Cr, ⁵⁵Fe, ⁵⁷Ni, ⁵⁰Sc, ⁵²V, ⁵⁴Mn, ⁵⁶Co; calculated levels, μ, S for one-nucleon transfer. Shell model.

doi: 10.1143/PTP.46.439
Citations: PlumX Metrics

1970HS02      Nucl.Phys. A151, 243 (1970)

S.T.Hsieh, H.Horie

Non-Normal Parity States in A = 15, 14 and 13 Nuclei

NUCLEAR STRUCTURE ^13,15C, ^14,15N; calculated non-normal- parity states. Shell model.

doi: 10.1016/0375-9474(70)90277-0
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1969AR11      Phys.Letters 30B, 14 (1969)

K.Arita, H.Horie

Shell Model Calculation of the Septuplet in ²⁰⁹Bi

NUCLEAR STRUCTURE ²⁰⁹Bi; calculated levels, wave functions.

doi: 10.1016/0370-2693(69)90273-1
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1968HO25      Proc.Intern.Conf.Nucl.Struct., Tokyo (1967), J.Sanada, Ed., Suppl.J.Phys.Soc.Japan 24, 119 (1968)

H.Horie, T.Oda, K.Ogawa

Effective Neutron-Proton Interactions in the Nuclei with N = 29

NUCLEAR STRUCTURE ⁴⁹Ca, ⁵¹Ti, ⁵³Cr, ⁵⁵Fe, ⁵⁷Ni, ⁵⁰Sc, ⁵²V, ^54,55Mn, ⁵⁶Co; calculated energy levels.

1955SH84      Phys.Rev. 100, 945 (1955)

R.Sherr, J.B.Gerhart, H.Horie, W.F.Hornyak

Decay Rates of C¹⁴, N¹⁴*, and O¹⁴

doi: 10.1103/PhysRev.100.945
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