Effect of Coriolis force on the shear viscosity of quark matter: A nonrelativistic description
arXiv:2303.16462 · doi:10.1103/PhysRevC.109.034913
Abstract
Shear viscosity becomes anisotropic in a rotating medium. It is discovered here that for rotating thermalized quantum systems such as those created in relativistic heavy-ion collisions, the coeffficient of shear viscosity breaks up into five independent components. Similar phenomena were also discovered for quark-gluon plasma in the presence of the magnetic field. Like the Lorentz force at a finite magnetic field, the Coriolis force also creates anisotropic viscosity at nonzero rotation. As a first approach, for simplicity, the calculations are done in the nonrelativistic prescription, with a future proposal to extend it toward a relativistic description. Introducing the Coriolis force term in relaxation time approximated Boltzmann transport equation, we have found different effective relaxation times along the parallel, perpendicular, and Hall directions in terms of actual relaxation time and rotating time period. Comparing the present formalism with the finite magnetic field picture, we have shown the equivalence of roles between the rotating and cyclotron time periods, where the rotating time period is inverse of twice the angular velocity.
11 pages, 5 figures
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- Shear Viscosity and Electrical Conductivity of Rotating Nuclear Medium in Hadron Resonance Gas and Nambu-Jona Lasinio Models
- Shear viscosity and electrical conductivity of rotating quark matter in Nambu--Jona-Lasinio Model
- Probing Rotational Dynamics of Quark Gluon Plasma via Global Vorticity
- Impact of spin polarization on transport and thermodynamic coefficients