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In this letter, based on Kubo’s formula and the QCD low energy theorem, we propose a direct formula for calculating the bulk viscosity of QCD at finite chemical potential and zero temperature. According to this formula, the bulk viscosity at finite is totally determined by the dressed quark propagator at finite . We then use a dynamical, confining Dyson-Schwinger equation model of QCD to calculate the bulk viscosity at finite . It is found that no sharp peak behavior of the bulk viscosity at finite is observed, which is quite different from that of the bulk viscosity at finite temperature.

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