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Progress of Theoretical Physics

One-Dimensional Many-Fermion System. I: Exact Solution in a Field Theoretical Framework

T. Kebukawa

Published May 1, 1985• 3 citations
Publisher

Abstract

The eigenvalue problem in a one-dimensional system of many fermions interacting via a delta-function potential is solved exactly in a field theoretical framework. Simultaneous eigenstates of spin and energy are represented in a systematic and compact form, that is, in such a form that the orbital and spin eigenfunctions are unified in harmony without the aid of Young’s tableau. The eigenstate and energy eigenvalue are specified by two sets of quantum numbers, particle momenta and spin momenta, besides two eigenvalues of a total spin angular momentum and its z-component. It is shown that for given particle momenta and spin momenta the energy eigenvalue is given by the solutions of coupled equations.

DOI
10.1143/ptp.73.1098

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The eigenvalue problem in a one-dimensional system of many fermions interacting via a delta-function potential is solved exactly in a field theoretical framework. Simultaneous eigenstates of spin and energy are represented in a systematic and compact form, that is, in such a form that the orbital and spin eigenfunctions are unified in harmony without the aid of Young’s tableau. The eigenstate and energy eigenvalue are specified by two sets of quantum numbers, particle momenta and spin momenta, besides two eigenvalues of a total spin angular momentum and its z-component. It is shown that for given particle momenta and spin momenta the energy eigenvalue is given by the solutions of coupled equations.
For a given eigenvalue of the square of the total spin operator, the spin eigenvectors with various eigenvalues of the z-component are obtained systematically by successive operations of the spin lowering operator on the eigenvector proposed in a previous paper for a one-dimensional many-fermion system with delta-function potential. The property of the spin eigenvector under the operation of the spin raising operator is investigated to clarify the mechanism how it has the given eigenvalue of the square of the total spin operator. It is shown that the spin eigenvector can be modified in various forms under some condition presented in the previous paper.
Dans le cadre de la theorie du champ, on resout exactement le probleme aux valeurs propres dans un systeme de fermions a 1 dimension interagissant par un potentiel en fonction delta. Les etats propres de spin et d'energie sont representes sous une forme systematique et compacte. Les etats propres et les valeurs propres de l'energie sont specifies par deux ensembles de nombres quantiques, les moments de particule et les moments de spin, entre deux valeurs propres d'un moment angulaire de spin total et sa composante z