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NSR database version of April 27, 2024.

Search: Author = S.Jang

Found 17 matches.

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1993JA02      Phys.Rev. C47, 286 (1993)

S.Jang

Coulomb Polarizability of the Deuteron and the E1 Capture Mechanism in the ⁴He(d, γ)⁶Li Reaction

NUCLEAR REACTIONS ⁴He(d, γ), E not given; calculated E1 vs E2 transition relative intensity; deduced Coulomb polarization of deuteron role.

doi: 10.1103/PhysRevC.47.286
Citations: PlumX Metrics

1987JA10      Phys.Rev. C36, 1587 (1987)

S.Jang, A.Bouyssy

Nuclear Elasticity Applied to Giant Resonances of Fast rotating Nuclei

NUCLEAR STRUCTURE A=150; calculated isoscalar giant resonance features. Fast rotating nuclei, nuclear elasticity model.

doi: 10.1103/PhysRevC.36.1587
Citations: PlumX Metrics

1986JA01      Phys.Rev. C33, 352 (1986)

S.Jang

Elastic Vibrational Approach to Giant Resonances of Deformed Nuclei

NUCLEAR STRUCTURE A=50-250; calculated giant multipole resonances. Giant monopole, quadrupole mode coupling, deformed nuclei.

doi: 10.1103/PhysRevC.33.352
Citations: PlumX Metrics

1985JA03      Nucl.Phys. A436, 397 (1985)

S.Jang, Z.Szymanski

Two-Fluid Model Description of Isovector Giant Resonances in Fast Rotating Nuclei

NUCLEAR STRUCTURE ²⁴Mg, ⁹⁰Zr, ^158,160Yb, ¹⁶⁴Er, ¹⁵⁴Sm; calculated isovector GDR frequencies. Two-fluid model.

doi: 10.1016/0375-9474(85)90076-4
Citations: PlumX Metrics

1985YA13      Phys.Lett. 163B, 55 (1985)

C.Yannouleas, S.Jang, Ph.Chomaz

A Second RPA Interpretation for the Widths of High Excitation Energy Structures in Heavy-Ion Collisions

NUCLEAR REACTIONS ²⁰⁸Pb(⁴⁰Ar, X), (²⁰Ne, X), E not given; calculated fragment spectral structure widths. Second RPA method.

doi: 10.1016/0370-2693(85)90191-1
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1980JA13      Nucl.Phys. A344, 315 (1980)

S.Jang, B.Sorensen

The (α, ⁶He) Reaction and Other Two-Neutron Transfer Reactions Leading to ²⁴Mg and ¹⁵²Sm

NUCLEAR REACTIONS ²⁶Mg(α, ⁶He), E=35.5, 40 MeV; ¹⁵⁴Sm(α, ⁶He), E=49.7 MeV; ²⁶Mg(p, t), E=27 MeV; ²⁶Mg(¹⁶O, ¹⁶O), E=60 MeV; analyzed σ(θ). ²⁴Mg levels deduced population mechanism. Deformed nucleus model, direct, multistep inelastic processes.

doi: 10.1016/0375-9474(80)90681-8
Citations: PlumX Metrics

1979BR15      J.Phys.(London) G5, 1249 (1979)

F.Brut, N.Mankoc-Borstnik, S.Jang

High-Spin States in ²³Na Obtained by Approximate Microscopic Methods Compared with Shell-Model Calculations

NUCLEAR STRUCTURE ²³Na; calculated levels, B(E2), B(M1), quadrupole moment. Generator coordinate, projected Hartree-Fock methods. Preedom-Wildenthal interaction, rotational structure.

doi: 10.1088/0305-4616/5/9/009
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1979BR22      J.Phys. (London) G5, 1249 (1979)

F.Brut, N.Mankoc-Borstnik, S.Jang

High-Spin States in ²³Na Obtained by Approximate Microscopic Methods Compared with Shell-Model Calculations

NUCLEAR STRUCTURE ²³Na; calculated levels, B(E2), B(M1), branching. Intrinsic quadrupole moment. Generator coordinate, projected Hartree-Fock methods.

doi: 10.1088/0305-4616/5/9/009
Citations: PlumX Metrics

1979MA27      Nucl.Phys. A325, 100 (1979)

N.Mankoc-Borstnik, F.Brut, S.Jang

Some Insight into the Structure of the Nuclei ¹⁹F, ¹⁹Ne, ²¹Ne, ²¹Na, ²³Na and ²³Mg Through the Generator Coordinate Method and the Projected Hartree-Fock Method

NUCLEAR STRUCTURE ^19,21Ne, ^21,23Na, ²³Mg, ¹⁹F; calculated electromagnetic properties for even-parity states. Generator coordinate method, mixed projected Hartree-Fock determinants.

doi: 10.1016/0375-9474(79)90155-6
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1978BR21      Nucl.Phys. A304, 429 (1978)

F.Brut, N.Mankoc-Borstnik, S.Jang

A Study of Even-Parity States of the Nuclei ¹⁹F, ²¹Ne and ²³Na with the Generator Coordinate Method and with Mixing of Projected Hartree-Fock Determinants in Comparison with Complete Diagonalization

NUCLEAR STRUCTURE ¹⁹F, ²¹Ne, ²³Na; calculated levels, B(λ), μ, quadrupole moment.

doi: 10.1016/0375-9474(78)90243-9
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1978BR26      Phys.Lett. 77B, 355 (1978)

F.Brut, S.Jang

Shape-Mixing in A-27 Nuclei

NUCLEAR STRUCTURE ²⁷Al, ²⁷Si; calculated structure.

doi: 10.1016/0370-2693(78)90576-2
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1976BR26      Phys.Rev. C14, 1638 (1976)

F.Brut, S.Jang

Application of the Projected Hartree-Fock Method to Rotational Motion in 1p-Shell Odd-A Nuclei

NUCLEAR STRUCTURE ⁷Li, ⁹Be, ¹¹B, ¹³N; calculated levels, μ, B(λ), moments of inertia. Projected Hartree-Fock method, cranking model.

doi: 10.1103/PhysRevC.14.1638
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1975CA08      Nucl.Phys. A243, 349 (1975)

J.F.Cavaignac, S.Jang, D.H.Worledge

Study of ¹¹B(p, p') in a Core-Hole Coupling Scheme

NUCLEAR REACTIONS ¹¹B(p, p'), E=30 MeV; measured σ(Ep', θ). ¹¹B deduced levels. Enriched ¹¹B diborane gas target.

doi: 10.1016/0375-9474(75)90253-5
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1972BO23      Nucl.Phys. A189, 334 (1972)

J.P.Boisson, S.Jang

Direct and Semi-Direct Radiative Capture of Nucleons in Deformed Nuclei

NUCLEAR REACTIONS ¹⁶⁰Gd, ¹⁵⁹Tb, ²⁰⁸Pb, ²³⁸U(n, γ), E=14 MeV; calculated σ(Eγ).

doi: 10.1016/0375-9474(72)90299-0
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1968GR07      J.Phys.(Paris) 29, 141 (1968)

J.Graff, G.Chouraqui, M.Port, J.M.Thirion, S.Jang, T.Muller

Desexcitation Electromagnetique des Niveaux a 11, 89 et 12, 28 MeV de ²²Ne

NUCLEAR STRUCTURE ²²Ne, ¹⁸O; measured not abstracted; deduced nuclear properties.

doi: 10.1051/jphys:01968002902-3014100
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1967YO03      Phys.Letters 24B, 9 (1967)

J.Yoccoz, S.Jang

T-Forbidden Electric Dipole Transition in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90321-8
Citations: PlumX Metrics

1967YO04      Nucl.Phys. A92, 505 (1967)

J.Yoccoz, S.Jang

Excitation Particule-Trou et Impurete du Spin Isobarique

doi: 10.1016/0375-9474(67)90629-X
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