The drag force on a heavy quark in a rotating finite-density holographic plasma is purely tangential and anisotropic, with worldsheet regularity fixing the renormalised transverse force and selecting a co-rotating equilibrium in the equal-spin sector.
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Anisotropic drag force in finite-density QGP from charged rotating 5D black holes
The drag force on a heavy quark in a rotating finite-density holographic plasma is purely tangential and anisotropic, with worldsheet regularity fixing the renormalised transverse force and selecting a co-rotating equilibrium in the equal-spin sector.