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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 />

◮ Define again thermal Green’s function<br />

[ ]<br />

G F (x, y; τ, 0) = Tr<br />

{ˆρT τ ˆψ(x, τ) ˆψ(y, }<br />

0)<br />

◮<br />

This time field operators anticommute!<br />

◮ Using cyclic property of the trace...<br />

{<br />

G F (x, y; τ, 0) = Z −1 Tr e −βĤe }<br />

βĤ ˆψ(y, 0)e −βĤ ˆψ(x, τ)<br />

}<br />

= Z −1 Tr<br />

{e −βĤ ˆψ(y, β) ˆψ(x, τ)<br />

= −Z −1 Tr<br />

{e −βĤT [<br />

τ ˆψ(x, τ) ˆψ(y, β) ]}<br />

= −G F (x, y; τ, β)<br />

logo<br />

Aleksi Vuorinen, CERN<br />

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

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