Relativistic transport theory of N, Δand N^{*}(1440) interacting through , and mesons
arXiv:nucl-th/9709047 · doi:10.1103/PhysRevC.57.1938
Abstract
A self-consistent relativistic integral-differential equation of the Boltzmann-Uehling-Uhlenbeck-type for the (1440) resonance is developed based on an effective Lagrangian of baryons interacting through mesons. The closed time-path Green's function technique and semi-classical, quasi-particle and Born approximations are employed in the derivation. The non-equilibrium RBUU-type equation for the (1440) is consistent with that of nucleon's and delta's which we derived before. Thus, we obtain a set of coupled equations for the , and (1440) distribution functions. All the (1440)-relevant in-medium two-body scattering cross sections within the , and (1440) system are derived from the same effective Lagrangian in addition to the mean field and presented analytically, which can be directly used in the study of relativistic heavy-ion collisions. The theoretical prediction of the free cross section is in good agreement with the experimental data. We calculate the in-medium , and cross sections in cold nuclear matter up to twice the nuclear matter density. The influence of different choices of the coupling strengths, which can not be obtained through fitting certain experimental data, are discussed. The results show that the density dependence of predicted in-medium cross sections are sensitive to the coupling strengths used. An evident density dependence will appear when a large scalar coupling strength of is assumed.
64 pages, Latex, 13 PostScript figures included
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Cited by in corpus (9)
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