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Springer eBooks

Calculation of Critical Exponents from Field Theory

Jean Zinn‐Justin

Published Jan 1, 1982• 2 citations
Publisher
DOI
10.1007/978-1-4613-3347-0_15

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We use field theory to calculate the critical exponents ${\ensuremath{\eta}}_{l2},$ ${\ensuremath{\eta}}_{l4},$ ${\ensuremath{\nu}}_{l2},$ and ${\ensuremath{\nu}}_{l4}$ for the Lifshitz point (LP) with m=2m=2m=2 and m=6m=6m=6. We were motivated by an old controversy on the order ${\ensuremath{\epsilon}}^{2}$ corrections for the exponents of this multicritical point. In a previous paper, we studied the renormalization of the theory that describes the LP and derived expressions for the exponents and scaling relations that hold to all orders in perturbation. In this work we concentrate on the calculation of the Feynman diagrams that are involved in the determination of the exponents and present our results for the exponents to order ${\ensuremath{\epsilon}}^{2}.$ The evaluation of these diagrams, due to a free propagator that contains a quartic term in the momentum and is not rotationally invariant, requires special techniques that are presented in detail in the appendixes.
We use a regularized (ϕ2)2 field theory for the determination of the critical exponents γ and ν in three dimensions. The regularization is done by a Gaussian propagator. This enables any order in g for any correlation function to be easily calculated but introduces a second expansion parameter. In spite of the difficulties encountered when dealing with double series, we obtain values for the critical exponents in good agreement with those found with the renormalized theory. This and the discussion we give of the link between the renormalized theory and our model illustrate the concept of universality in critical phenomena.