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85037232575
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A more complete expression is (Formula presented) satisfying the dynamic screening for (Formula presented) and the Debye wave number for (Formula presented) This simple form is very closed to the self-consistent value calculated in Ref
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A more complete expression is (Formula presented) satisfying the dynamic screening for (Formula presented) and the Debye wave number for (Formula presented) This simple form is very closed to the self-consistent value calculated in Ref. 15.
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21
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5344229956
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M. Chevallier, A. Clouvas, N. V. de Castro Faria, B. Farizon Mazuy, M. J. Gaillard, J. C. Poizat, J. Remillieux, and J. Désesquelles, Phys. Rev. A 41, 1738 (1990).PLRAAN
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Remillieux, J.7
Désesquelles, J.8
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26
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85037190130
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If (Formula presented) were required to be unitary in everywhere, it would mean that (Formula presented) in Eq. (4) is changed to (Formula presented) where (Formula presented). This would imply the relaxation of the energy conservation in the Fermi golden rule to permit two-particle final states which do not conserve the energy (of course the whole many-electron system must conserve the energy)
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If (Formula presented) were required to be unitary in everywhere, it would mean that (Formula presented) in Eq. (4) is changed to (Formula presented) where (Formula presented). This would imply the relaxation of the energy conservation in the Fermi golden rule to permit two-particle final states which do not conserve the energy (of course the whole many-electron system must conserve the energy).
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