123,655 research outputs found

    Quantum Mechanical Embedding of Spinning Particle and Induced Spin-connection

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    This paper introduces the way of the embedding of spinning particle quantum mechanically. Schr\"odinger equation on its submanifold obtains the gauge field as spin connection, and it reduces to the ones obtained by Ohnuki and Kitakado when we consider S2S^2 in R3R^3. PACS numbers: 03.65Comment: 6 pages, No figures, Latex, Some parts are explained more clearly, and 1page is adde

    Spectral and formal stability criteria of spatially inhomogeneous stationary solutions to the Vlasov equation for the Hamiltonian mean-field model

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    Stability of spatially inhomogeneous solutions to the Vlasov equation is investigated for the Hamiltonian mean-field model to provide the spectral stability criterion and the formal stability criterion in the form of necessary and sufficient conditions. These criteria determine stability of spatially inhomogeneous solutions whose stability has not been decided correctly by using a less refined formal stability criterion. It is shown that some of such solutions can be found in a family of stationary solutions to the Vlasov equation, which is parametrized with macroscopic quantities and has a two-phase coexistence region in the parameter space.Comment: 17 pages, 4 figures, text modified, section VE added, references added, Accepted for publication in Phys. Rev.

    Algebraic construction of spherical harmonics

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    The angular wave functions for a hydrogen atom are well known to be spherical harmonics, and are obtained as the solutions of a partial differential equation. However, the differential operator is given by the Casimir operator of the SU(2)SU(2) algebra and its eigenvalue l(l+1)2l(l+1) \hbar^2, where ll is non-negative integer, is easily obtained by an algebraic method. Therefore the shape of the wave function may also be obtained by extending the algebraic method. In this paper, we describe the method and show that wave functions with different quantum numbers are connected by a rotational group in the cases of l=0l=0, 1 and 2.Comment: 9pages, 13figure
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