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For example, these functions could be obtained from a calculation in a quasidiabatic representation, as discussed in Sec..
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For example, these functions could be obtained from a calculation in a quasidiabatic representation, as discussed in Sec..
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This distinction arises because the Feynman paths that contribute to the kernel wind a finite number of times around the CI in a time-independent scattering state, but an infinite number of times in a time-independent bound state; see Ref..
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This distinction arises because the Feynman paths that contribute to the kernel wind a finite number of times around the CI in a time-independent scattering state, but an infinite number of times in a time-independent bound state; see Ref..
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This argument implies that, for any wave function in a N -dimensional coordinate space, one can pick an N-2 dimensional hyperline connecting an arbitrary set of points in the space, and then decompose the wave function into contributions with different winding numbers n. In general, however, the n will have no meaningful physical interpretation, and the procedure would thus amount to an arbitrary decomposition of the wave function.
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This argument implies that, for any wave function in a N -dimensional coordinate space, one can pick an N-2 dimensional hyperline connecting an arbitrary set of points in the space, and then decompose the wave function into contributions with different winding numbers n. In general, however, the n will have no meaningful physical interpretation, and the procedure would thus amount to an arbitrary decomposition of the wave function.
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