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NSR database version of April 27, 2024.

Search: Author = J.M.Hu

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1999BR06      Phys.Rev. C59, 767 (1999)

U.Brosa, H.-H.Knitter, T.-S.Fan, J.-M.Hu, S.-L.Bao

Systematics of Fission-Channel Probabilities

NUCLEAR STRUCTURE ^234,236,239U, ^232,233Th, ²³⁸Np, ^240,242Pu; analyzed fission channel probabilities; deduced barrier parameters.

doi: 10.1103/PhysRevC.59.767
Citations: PlumX Metrics

1995FA14      Nucl.Phys. A591, 161 (1995); Erratum Nucl.Phys. A606, 607 (1996)

T.-S.Fan, J.-M.Hu, S.-L.Bao

Study of Multichannel Theory for the Neutron Induced Fissions of Actinide Nuclei

NUCLEAR REACTIONS ²³⁵U(n, F), E=thermal, 0.5-6 MeV; ²³²Th(n, F), E=1.38-5.6 MeV; ²³³U(n, F), E=thermal, 0.45=5.5 MeV; ²³⁸U(n, F), E=1.3-5.3 MeV; ²³⁷Np(n, F), E=0.8, 5.5 MeV; ²³⁹Pu(n, F), E=thermal, 5.5 MeV; ²⁴⁰Pu(n, F), E=0.85, 4.9 MeV; ²⁴¹Pu(n, F), E=0.3-5 MeV; ²⁴²Pu(n, F), E=0.7, 4.9 MeV; analyzed fission fragment mass yield distributions, total kinetic energy, neutron multiplicities; deduced channel probability incident energy dependence.

doi: 10.1016/0375-9474(95)00193-5
Citations: PlumX Metrics

1989WA12      J.Phys.(London) G15, 829 (1989)

F.-C.Wang, J.-M.Hu

A Study of the Multimode Fission Model

NUCLEAR REACTIONS, ICPND ²³⁷Np, ²⁴⁵Cm, ²³⁵U, ²⁵⁷Fm(n, F), E=thermal; ^233,235,238U, ²³²Th, ^{239,240,241,242}Pu(n, F), E=fast; ²³⁰Th, ²³³U(α, F), E=25.7 MeV; ²²⁶Ra(p, F), E=13 MeV; calculated fission fragment yield vs mass. Multi-mode fission model.

RADIOACTIVITY ²⁵⁸Fm, ²⁵²Cf(SF); analyzed fission fragment yield vs mass; deduced minimum potential positions. Multi-mode fission model.

NUCLEAR STRUCTURE ²⁵⁸Fm, ²⁵²Cf, ²²⁷Ac; calculated potential contours. Multi-mode fission model.

doi: 10.1088/0954-3899/15/6/013
Citations: PlumX Metrics

1986HU08      Radiat.Eff. 95, 175 (1986)

J.-M.Hu, C.-K.Zheng

A Proposed Macroscopic Model of the Nucleus

NUCLEAR STRUCTURE A=40-240; calculated densities, rms radii; deduced mass formula. Macroscopic model.

doi: 10.1080/00337578608208689
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