-meson properties at finite nuclear density
arXiv:nucl-th/9801055 · doi:10.1103/PhysRevC.58.1078
Abstract
We calculate the momentum dependence of the -meson selfenergy based on the dispersion relation for the scattering amplitude ) at low nuclear density. The imaginary part of is determined from the optical theorem, while the total cross section is obtained within the VDM at high energy and within the resonance model at low energy. Our numerical results indicate a sizeable broadening of the -meson width in the medium especially for low relative momenta while the real part of the selfenergy is found to change its sign and becomes repulsive already at momenta above 100 MeV/c. Extrapolating to nuclear saturation density we find a dropping of the -mass for 0 in line with the QCD sumrule analysis of Hatsuda while at high energy an increase of the -mass in line with the prediction by Eletsky and Joffe is obtained. However, when including a broadening of the baryonic resonances in the medium, the -meson mass shift at 0 becomes slightly repulsive whereas the width increases substantially.
20 pages, LaTeX, including 7 ps-figures, UGI-97-4, revised version, to be pub. in Phys. Rev. C
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