Environmentally Friendly Renormalization
arXiv:hep-th/9310198 · doi:10.1142/S0217751X94001151
Abstract
We analyze the renormalization of systems whose effective degrees of freedom are described in terms of fluctuations which are ``environment'' dependent. Relevant environmental parameters considered are: temperature, system size, boundary conditions, and external fields. The points in the space of \lq\lq coupling constants'' at which such systems exhibit scale invariance coincide only with the fixed points of a global renormalization group which is necessarily environment dependent. Using such a renormalization group we give formal expressions to two loops for effective critical exponents for a generic crossover induced by a relevant mass scale . These effective exponents are seen to obey scaling laws across the entire crossover, including hyperscaling, but in terms of an effective dimensionality, $d\ef=4-\gl$, which represents the effects of the leading irrelevant operator. We analyze the crossover of an model on a dimensional layered geometry with periodic, antiperiodic and Dirichlet boundary conditions. Explicit results to two loops for effective exponents are obtained using a [2,1] Padé resummed coupling, for: the ``Gaussian model'' (), spherical model (), Ising Model (), polymers (), XY-model () and Heisenberg () models in four dimensions. We also give two loop Padé resummed results for a three dimensional Ising ferromagnet in a transverse magnetic field and corresponding one loop results for the two dimensional model. One loop results are also presented for a three dimensional layered Ising model with Dirichlet and antiperiodic boundary conditions. Asymptotically the effective exponents are in excellent agreement with known results.
76 pages of Plain Tex, Postscript figures available upon request from [email protected], preprint numbers THU-93/14, DIAS-STP-93-19
Cited by in corpus (29)
- Non-Perturbative Renormalization Flow in Quantum Field Theory and Statistical Physics
- Quantum Fluctuations, Decoherence of the Mean Field, and Structure Formation in the Early Universe
- Stochastic dynamics of correlations in quantum field theory: From Schwinger-Dyson to Boltzmann-Langevin equation
- Stochastic Behavior of Effective Field Theories Across Threshold
- Defect Formation and Critical Dynamics in the Early Universe
- Field Theory Entropy, the -theorem and the Renormalization Group
- Kaluza-Klein Thresholds and Regularization (In)dependence
- Analysis of the Wilsonian Effective Potentials in Dynamical Chiral Symmetry Breaking
- Dimensional Crossover and Effective Exponents
- Renormalization group and nonequilibrium action in stochastic field theory
- Roughening of the (1+1) interfaces in two-component surface growth with an admixture of random deposition
- Modular invariance, lattice field theories and finite size corrections
- Renormalization and resummation in finite temperature field theories
- Scaling Laws and Effective Dimension in Lattice SU(2) Yang-Mills Theory with a Compactified Extra Dimension
- Why Two Renormalization Groups are Better than One
- Renormalization of 2PI resummation: a renormalization scheme approach
- Critical Behavior of phi^4-Theory from the Thermal Renormalization Group
- Scheme Independence of Blocking Transformation in Finite-Temperature Renormalization Group
- Thermal Renormalization Group-Equations and the Phase-Transition of Scalar O(N)-Theories
- Renormalization in momentum dependent resummations
- An Analytic Equation of State for Ising-like Models
- The Thermal Renormalization Group for Fermions, Universality, and the Chiral Phase-Transition
- Dimensional Crossover in the Large N Limit
- Crossover scaling functions and an extended minimal subtraction scheme
- Regge Behaviour from an Environmentally Friendly Renormalization Group
- Flow of the Coarse Grained Free Energy for Crossover Phenomena
- Dimensional Reduction, Hard Thermal Loops and the Renormalization Group
- An ab initio Calculation of the Universal Equation of State for the O(N) Model
- Two-Loop Crossover Scaling Functions of the O(N) Model