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We calculate the spectral function of the meson in nuclear matter. The calculation is performed in the {\it low density} approximation, where the in-medium self energy is completely determined by the vacuum forward scattering amplitude. This amplitude is derived from a relativistic resonance model. In comparison to previous non-relativistic calculations we find a much weaker momentum dependence of , especially in the transverse channel. Special attention is paid to uncertainties in the model. Thus, we compare the impact of different coupling schemes for the interaction on the results and discuss various resonance parameter sets.

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