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Nuclear Physics B

Phase transitions and dimensional reduction

Denjoe O’Connor, Christopher Rhodes Stephens

Published Aug 1, 1991• 50 citations
Publisher
DOI
10.1016/0550-3213(91)90405-m

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We consider phase transitions in the presence of random magnetic fields, with long-range correlations such that $〈h(0)h(r)〉\ensuremath{\sim}\frac{1}{{r}^{d\ensuremath{-}\ensuremath{\sigma}}}$. The upper critical dimension is $6+\ensuremath{\sigma}$. A superspace renormalization-group calculation is carried out to order ${\ensuremath{\epsilon}}^{2}$, where $\ensuremath{\epsilon}=6+\ensuremath{\sigma}\ensuremath{-}d$. To order $\ensuremath{\epsilon}$, the critical properties are that of a pure system in $d\ensuremath{-}2\ensuremath{-}\ensuremath{\sigma}$ dimensions. This dimensional reduction is also justified by physical arguments concerning the lower critical dimensionality, and the hyperscaling relationship. However, it fails at order ${\ensuremath{\epsilon}}^{2}$.