Revisiting the local potential approximation of the exact renormalization group equation
arXiv:1307.3679 · doi:10.1016/j.nuclphysb.2013.08.008
Abstract
The conventional absence of field renormalization in the local potential approximation (LPA) --implying a zero value of the critical exponent η-- is shown to be incompatible with the logic of the derivative expansion of the exact renormalization group (RG) equation. We present a LPA with η\neq 0 that strictly does not make reference to any momentum dependence. Emphasis is made on the perfect breaking of the reparametrization invariance in that pure LPA (absence of any vestige of invariance) which is compatible with the observation of a progressive smooth restoration of that invariance on implementing the two first orders of the derivative expansion whereas the conventional requirement (η=0 in the LPA) precluded that observation.
Final version, some misprints corrected
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- The fate of non-polynomial interactions in scalar field theory
- The local potential approximation in the background field formalism
- Self-consistent renormalization group approach to continuous phase transitions in alloys. Application to ordering in -brass
- Effective medium approach in the renormalization group theory of phase transitions
- Universal scaling dimensions for highly irrelevant operators in the Local Potential Approximation
- Exact renormalization group equation for lattice Ginzburg-Landau models adapted to the solution in the local potential approximation