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Linear Canonical Transformations and Interacting n-Particle Systems,2,..., n denoting the particle number. Among the linear point transformations acting on these coordinates there are two commuting subgroups of transformations. The elements of the first one are given by product matrices M. × I. where the 3 × 3 matrix M. acts on the vector components. The elements of

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脊椎動(dòng)物

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Interaction of Composite Nucleon Systems with Internal Shell Structure,lytic properties of the overlap matrix between single-particle states. By a modification of the single-particle basis, we arrive at a new biorthogonal basis which leads to a simpler form of the matrix .. This modification is implemented through the generalized Weyl operators introduced in section 4.

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Configurations of Three Simple Composite Particles and the Structure of Nuclei with Mass Numbers A reaction theory, but the problems involved become enormous when several channels are open. Therefore things are simplified drastically if in a quasibound approach square integrable functions are used only. Then the A-body hamiltonian can be diagonalized in order to derive observable quantities from

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Sleep-Paralysis

Composite Nucleon Systems and their Interaction,quations which govern this state. These integral equations are characterized by kernels of interaction and normalization operators which depend on the choice of the internal states, on the choice of the orbital partition and on the nucleon-nucleon interaction. The kernels of these operators are expr

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Interaction of Composite Nucleon Systems with Internal Shell Structure,omposition and compute its eigenfunctions and eigenvalues. The eigenvalues reflect the action of the Pauli principle on the composite particle interaction as a function of the relative excitation and the mass numbers of the fragments. In section 8.5, we study the configuration s.p. + s.p. which cove

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