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NSR database version of May 8, 2024.

Search: Author = M.E.Faber

Found 9 matches.

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1984FA13      Acta Phys.Pol. B15, 949 (1984)

M.E.Faber, M.Ploszajczak, K.Junker

Shape and Fission Instability of Rotating Nuclei at Finite Temperatures

NUCLEAR STRUCTURE ²³⁸U; calculated fission barrier, deformation, isentropic energy surfaces, shell energy, thermal particle-hole excitation energy vs deformation. ²¹⁰Po; calculated first, second fission barriers. Rotating liquid drop model.

1983FA10      Phys.Lett. 127B, 5 (1983)

M.E.Faber, J.L.Egido, P.Ring

The Giant Resonance in Hot Rotating Nuclei

NUCLEAR REACTIONS ^158,164Er(γ, X), E=10-20 MeV; calculated dipole absorption σ(E). Linear response theory, hot rotating nuclei.

NUCLEAR STRUCTURE ^158,164Er; calculated GDR energy, splitting vs angular momentum, temperature. Linear response theory, hot rotating nuclei.

doi: 10.1016/0370-2693(83)91618-0
Citations: PlumX Metrics

1982MA32      Nuovo Cim. 70A, 62 (1982)

H.Markum, M.E.Faber, A.Ansari, G.Eder, A.Faessler

Investigation of Pairing Correlations in High-Spin States by HBF and BCS Approach

NUCLEAR STRUCTURE ¹⁵⁰Gd; calculated total energy, deformation energy vs total angular momentum. HFB, modified BCS formalisms.

1982PL01      Phys.Rev. C25, 1538 (1982)

M.Ploszajczak, M.E.Faber

Competition between Fission and Neutron Emission at High Spins and Excitation Energies

NUCLEAR STRUCTURE ²¹⁰Po, ²³²U; analyzed Γf/Γn; deduced shell effects, angular momentum, saddle point deformation. Statistical theory.

doi: 10.1103/PhysRevC.25.1538
Citations: PlumX Metrics

1981BE41      Phys.Scr. 24, 200 (1981)

T.Bengtsson, M.E.Faber, G.Leander, P.Moller, M.Ploszajczak, I.Ragnarsson, S.Aberg

Some Properties of Superdeformed Nuclei

NUCLEAR STRUCTURE ¹⁵²Dy; calculated potential, shell energy surfaces; ^90,92Zr, ⁹⁶Ru; calculated potential energy vs deformation; ⁹⁶Ru; calculated liquid drop model energy. Anisotropic harmonic oscillator potential. A ≈ 100; deduced superdeformed properties. A ≈ 150; deduced superdeformed properties.

doi: 10.1088/0031-8949/24/1B/016
Citations: PlumX Metrics

1981BO12      J.Phys.(London) G7, 321 (1981)

N.Bottges, A.Faessler, M.E.Faber

Collective Transitions in Nuclei with 'Rotations' around the Symmetry Axis

NUCLEAR STRUCTURE ¹⁵⁴Er; calculated yrast line, B(E2); ^150,152Gd, ^152,154Dy, ^152,156Er; calculated B(E2); deduced γ-vibrations around axially symmetric equilibruim deformation. BCS, number projection before variation.

doi: 10.1088/0305-4616/7/3/008
Citations: PlumX Metrics

1981FA04      Phys.Rev. C24, 1047 (1981)

M.E.Faber

Influence of Angular Momentum on the Mass Distribution of Heavy-Ion-Induced Fission

NUCLEAR STRUCTURE ²⁰⁵At; calculated deformation energy surfaces; deduced fusion-fission event mass distribution width. Heated rotating nuclei, Strutinsky method.

doi: 10.1103/PhysRevC.24.1047
Citations: PlumX Metrics

1981FA05      Phys.Scr. 24, 189 (1981)

M.E.Faber, M.Ploszajczak

Shell Structure in Superdeformed Light Nuclei (A < 40) at High Rotational Frequencies

NUCLEAR STRUCTURE ²⁴Mg, ^26,27Al, ^28,30Si; calculated deformation, superdeformation energy surfaces. Cranking Strutinsky model, Saxon-Woods potential.

doi: 10.1088/0031-8949/24/1B/015
Citations: PlumX Metrics

1980FA15      Z.Phys. A297, 277 (1980)

M.E.Faber

The Mass Distribution Width of Heavy-Ion Fission for Various Composite Systems

NUCLEAR STRUCTURE ²⁰⁵At, ²²¹Pa; caculated rotating liquid drop energy; deduced fission barrier height, mass distribution width correlation.

doi: 10.1007/BF01892810
Citations: PlumX Metrics