Limit of vanishing regulator in the functional renormalization group
arXiv:2105.05778 · doi:10.1103/PhysRevD.104.076026
Abstract
The non-perturbative functional renormalization group equation depends on the choice of a regulator function, whose main properties are a "coarse-graining scale" and an overall dimensionless amplitude . In this paper we shall discuss the limit with fixed. This limit is closely related to the pseudo-regulator that reproduces the beta functions of the scheme, that we studied in a previous paper. It is not suitable for precision calculations but it appears to be useful to eliminate the spurious breaking of symmetries by the regulator, both for nonlinear models and within the background field method.
arXiv comment24 pages, 5 figures, 2 tables. Updated to match the published version
References in corpus (31)
- Exact evolution equation for the effective potential
- The Exact Renormalisation Group and Approximate Solutions
- Optimised Renormalisation Group Flows
- The nonperturbative functional renormalization group and its applications
- Flow Equations for N Point Functions and Bound States
- Derivative Expansion of the Exact Renormalization Group
- Bootstrapping Mixed Correlators in the 3D Ising Model
- Critical exponents from optimised renormalisation group flows
- Nonperturbative renormalization group approach to the Ising model: a derivative expansion at order
- Flow Equations and BRS Invariance for Yang-Mills Theories
- Mind The Gap
- Perturbative renormalization and infrared finiteness in the Wilson renormalization group: the massless scalar case
- Convergence of Non-Perturbative Approximations to the Renormalization Group
- Renormalization flow of Yang-Mills propagators
- Precision calculation of critical exponents in the universality classes with the nonperturbative renormalization group
- The Heavy Quark Potential from Wilson's Exact Renormalization Group
- Large N and the renormalization group
- Two loop results from one loop computations and non perturbative solutions of exact evolution equations
- Exact scheme independence at two loops
- Fixed points and the spontaneous breaking of scale invariance
- Scheme dependence and universality in the functional renormalization group
- Beta function and infrared renormalons in the exact Wilson renormalization group in Yang-Mills theory
- Conformal invariance in the nonperturbative renormalization group: a rationale for choosing the regulator
- Two-loop beta-function from the exact renormalization group
- Two loop results from the derivative expansion of the blocked action
- Functional Renormalization and
- Perturbative and non-perturbative aspects of the proper time renormalization group
- Renormalized Functional Renormalization Group
- Wilsonian Flow and Mass-Independent Renormalization
- Functional RG flow equation: regularization and coarse-graining in phase space
- Phase structure of a three-dimensional Yukawa model
Cited by in corpus (4)
- Dimensional regularization, Wilsonian RG, and the Naturalness/Hierarchy problem
- Nonvanishing gravitational contribution to matter beta functions for vanishing dimensionful regulators
- Tunneling with physics-informed RG flows in the anharmonic oscillator
- Functional renormalization group for p=2 like glassy matrices in the planar approximation: I. Vertex expansion at equilibrium