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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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Published in: | Annals of physics 2013-11, Vol.338, p.32-49 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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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. |
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ISSN: | 0003-4916 1096-035X |
DOI: | 10.1016/j.aop.2013.07.004 |