1991
DOI: 10.1103/physrevc.44.2456
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Relativistic mean-field kinetic equation: Collectives modes and symmetry breaking in nuclear matter

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Cited by 14 publications
(26 citation statements)
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“…The quantity A(K F , M * ) is the same integral discussed in Eqs. (9,10,11). At this point we can make the following approximation…”
Section: Isovector Responsementioning
confidence: 99%
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“…The quantity A(K F , M * ) is the same integral discussed in Eqs. (9,10,11). At this point we can make the following approximation…”
Section: Isovector Responsementioning
confidence: 99%
“…(13) and (14) by γ λ . After performing the traces, and we equate to zero both the real and imaginary parts of the result [10,11]. Furthermore, by Fourier transforming and integrating over four-momentum, we get the set of equations for the scalar and vector fluctuation of each species ( i = 1, 2 for proton, neutron respectively):…”
Section: Linear Response Equationsmentioning
confidence: 99%
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“…(3) by means of Eq.(4). As far as the term containing the vector field is concerned, by a simple substitution one can obtain a statistical average of only fermionic field operators [8]. Instead, because of the non-linear coupling of the σ field to the fermionic scalar density, the elimination of the scalar field in the last term of Eq.…”
Section: B the Truncation Scheme For Exchange Contributionsmentioning
confidence: 99%
“…quoted in [2][3][4] ). Including the Fock terms also the whole variety of processes in nuclear dynamics arising from the fermionic intrinsic degrees of freedom ( spin and isospin ), can be accounted for [8][9][10]. In principle, if the model is constructed self-consistently, the introduction of further meson fields with the corresponding constants for the coupling to nucleons appears to be less necessary.…”
Section: Introductionmentioning
confidence: 99%