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Relativistic distribution function for particles with spin at local thermodynamical equilibrium

We present an extension of relativistic single-particle distribution function for weakly interacting particles at local thermodynamical equilibrium including spin degrees of freedom, for massive spin 1/2 particles. We infer, on the basis of the global equilibrium case, that at local thermodynamical...

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Bibliographic Details
Published in:Annals of physics 2013-11, Vol.338, p.32-49
Main Authors: Becattini, F., Chandra, V., Del Zanna, L., Grossi, E.
Format: Article
Language:English
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Summary:We present an extension of relativistic single-particle distribution function for weakly interacting particles at local thermodynamical equilibrium including spin degrees of freedom, for massive spin 1/2 particles. We infer, on the basis of the global equilibrium case, that at local thermodynamical equilibrium particles acquire a net polarization proportional to the vorticity of the inverse temperature four-vector field. The obtained formula for polarization also implies that a steady gradient of temperature entails a polarization orthogonal to particle momentum. The single-particle distribution function in momentum space extends the so-called Cooper–Frye formula to particles with spin 1/2 and allows us to predict their polarization in relativistic heavy ion collisions at the freeze-out. •Single-particle distribution function in local thermodynamical equilibrium with spin.•Polarization of spin 1/2 particles in a fluid at local thermodynamical equilibrium.•Prediction of a new effect: a steady gradient of temperature induces a polarization.•Application to the calculation of polarization in relativistic heavy ion collisions.
ISSN:0003-4916
1096-035X
DOI:10.1016/j.aop.2013.07.004