Abstract

We investigate the in-medium properties of strange vector mesons (K∗K^* and Kˉ∗\bar K^*) in dense and hot nuclear matter based on chirally motivated models of the meson selfenergies. We parameterise medium effects as density or temperature dependent effective masses and widths, obtain the vector meson spectral functions within a Breit-Wigner prescription (as often used in transport simulations) and study whether such an approach can retain the essential features of full microscopic calculations. For μB≠0μ_B\ne 0 the medium corrections arise from Kˉ∗(K∗)N\bar K^* (K^*) N scattering and the Kˉ∗(K∗)→Kˉ(K)π\bar K^* (K^*) \to \bar K (K) π decay mode (accounting for in-medium Kˉ(K)\bar K (K) dynamics). We calculate the scattering contribution to the K∗K^* selfenergy based on the hidden local symmetry formalism for vector meson nucleon interactions, whereas for the Kˉ∗\bar K^* selfenergy we implement recent results from a selfconsistent coupled-channel determination within the same approach. For μB≃0μ_B\simeq 0 and finite temperature we rely on a phenomenological approach for the kaon selfenergy in a hot pionic medium consistent with chiral symmetry, and evaluate the Kˉ∗(K∗)→Kˉ(K)π\bar K^* (K^*) \to \bar K (K) π decay width. The emergence of a mass shift at finite temperature is studied with a dispersion relation over the imaginary part of the vector meson selfenergy.

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