Abstract
The principal goal of the theory of critical phenomena is to make quantitative predictions for universal features of critical behavior — critical exponents, universal ratios of critical amplitudes, equations of state, and so forth — as discussed in Section 1.1. (Non-universal features, such as critical temperatures, are of lesser interest.) The present status of the theory of critical phenomena is roughly the following:
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Non-rigorous renormalization-group calculations predict mean-field critical behavior for systems above their upper critical dimension d c (e.g. d c = 4 for short-range Ising-type models). For systems below their upper critical dimension (e.g. d = 3), RG methods predict exact scaling laws relating critical exponents, and give reasonably accurate numerical predictions of individual critical exponents (and other universal quantities).1
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Rigorous mathematical analysis has given a proof of (some aspects of) mean-field critical behavior for (certain) systems above their upper critical dimension (e.g. short-range Ising models for d > 4). For systems below their upper critical dimension, much less is known. Often one half of a scaling law can be proven as a rigorous inequality. Likewise, rigorous upper or lower bounds on individual critical exponents can in many cases be proven.
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© 1992 Springer-Verlag Berlin Heidelberg
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Fernández, R., Fröhlich, J., Sokal, A.D. (1992). Inequalities for critical exponents. In: Random Walks, Critical Phenomena, and Triviality in Quantum Field Theory. Texts and Monographs in Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-02866-7_14
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DOI: https://doi.org/10.1007/978-3-662-02866-7_14
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-662-02868-1
Online ISBN: 978-3-662-02866-7
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