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楼主: 新石器时代
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Amarjeet Shrama,Priyanshi,Chandi C. Mandal nucleons and introduce a partition of n to specify j occupation numbers (n. n. ... n.). Using these occupation numbers we pass from the coordinates x. x. ... x. of the single particles to j center coordinates z and n - j internal coordinates y. Next we specify the orbital state with respect to the
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Florence Wong,Tilman Sauerbruchlytic 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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Domenic A. Ciraulo,Richard Irwin Shaderreaction 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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