Nonperturbative Renormalization Group for the Landau-de Gennes Model
arXiv:1803.03683 · doi:10.1103/PhysRevB.98.014102
Abstract
We studied the nematic isotropic phase transition by applying the functional renormalization group to the Landau-de Gennes model. We derived the flow equations for the effective potential as well as the cubic and quartic "couplings" and the anomalous dimension. We then solved the coupled flow equations on a grid using Newton Raphson method. A first order phase transition is observed. We also investigated the nematic isotropic puzzle (the NI puzzle) in this paper. We obtained the NI transition temperature difference with sizable improvement over previous results.
arXiv comment8 pages, 8 figures in Revtex
References in corpus (18)
- Exact evolution equation for the effective potential
- Non-Perturbative Renormalization Flow in Quantum Field Theory and Statistical Physics
- Aspects of the Functional Renormalisation Group
- Optimised Renormalisation Group Flows
- Functional renormalization group approach to correlated fermion systems
- An Introduction to the Nonperturbative Renormalization Group
- Nonperturbative renormalization group approach to frustrated magnets
- Solving non-perturbative flow equations
- Baryon number fluctuations at finite temperature and density
- Multicritical behavior in models with two competing order parameters
- Functional renormalization group study of the two-flavor linear sigma model in the presence of the axial anomaly
- Equation of state and coarse grained free energy for matrix models
- Second-order and Fluctuation-induced First-order Phase Transitions with Functional Renormalization Group Equations
- Scaling functions for the O(4)-model in d=3 dimensions
- Functional Renormalization for Chiral and U_A(1) Symmetries at Finite Temperature
- Functional renormalization group approach to non-collinear magnets
- Fluctuation induced first order phase transition in U(n)xU(n) models using chiral invariant expansion of functional renormalization group flows
- Phase Transitions in liquid Helium 3