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Finite-temperature Field Theory - Theoretical Physics (TIFR)

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Basics of Statistical <strong>Physics</strong> and Thermodynamics<br />

Scalar fields at finite <strong>temperature</strong><br />

Interacting scalar fields<br />

Partition function for scalar field theory<br />

Non-interacting examples<br />

Brief note on fermions<br />

◮ For free Dirac fermions, going from QFT transition<br />

amplitude to finite-T partition function proceeds as above<br />

∫<br />

[ ∫ β ∫<br />

Z = D ¯ψDψ exp − dτ d 3 xL E<br />

],<br />

{<br />

}<br />

L = ¯ψ γ 0 ∂ τ − iγ i ∂ i + m ψ<br />

0<br />

◮ What about periodicity?<br />

◮ Spinor fields satisfy canonical anticommutation relations<br />

and are represented by Grassmann variables<br />

◮ Let’s try to repeat our proof of periodicity for bosonic<br />

fields...<br />

logo<br />

Aleksi Vuorinen, CERN<br />

<strong>Finite</strong>-<strong>temperature</strong> <strong>Field</strong> <strong>Theory</strong>

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