We investigate a system of two-dimensional interacting Brownian particles at finite density. In the continuum limit, we uncover a hidden symmetry under area-preserving diffeomorphism transformations. This symmetry leads to the conservation of local vorticity. By calculating the generating functional within the saddle-point plus Gaussian fluctuations approximation, we reveal the emergence of a $U(1)$ gauge symmetry. This emergent symmetry enables us to describe the dynamics of density fluctuations as a gauge theory. We solve the corresponding equations of motion for various local and non-local two-body potentials, demonstrating the presence of multiple dynamical regimes and associated dynamical phase transitions.
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Silvano et al. (2024) studied this question.
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