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Rotational Motion of Deformed Nuclei

V. A. Krutov

Open publisher page 29 citations

Abstract

Abstract Collective motion in the nucleus is defined as change of the density distribution of nuclear matter in time. On the basis of this definition the Hamiltonian of nuclear rotation is obtained with moments of inertia corresponding satisfactorily to experimental data. The theory is easily applied to nuclei with non‐axial equilibrium shape. For the latter the parameters of non‐axiality are considerably smaller than in the DAVYDOV‐FILIPPOV model.

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What this paper is about

Abstract Collective motion in the nucleus is defined as change of the density distribution of nuclear matter in time. On the basis of this definition the Hamiltonian of nuclear rotation is obtained with moments of inertia corresponding satisfactorily to experimental data. The theory is easily applied to nuclei with non‐axial equilibrium shape. For the latter the parameters of non‐axiality are considerably smaller than in the DAVYDOV‐FILIPPOV model.

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Available abstract

Abstract Collective motion in the nucleus is defined as change of the density distribution of nuclear matter in time. On the basis of this definition the Hamiltonian of nuclear rotation is obtained with moments of inertia corresponding satisfactorily to experimental data. The theory is easily applied to nuclei with non‐axial equilibrium shape. For the latter the parameters of non‐axiality are considerably smaller than in the DAVYDOV‐FILIPPOV model.

Key concepts: Physics, Moment of inertia, Hamiltonian (control theory), Collective motion, Classical mechanics, Nuclear matter, Rotation around a fixed axis, Nucleus

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