Effective potential in the BET formalism
arXiv:1104.1084 · doi:10.1103/PhysRevD.83.125016
Abstract
We calculate the one-loop effective potential at finite temperature for a system of massless scalar fields with quartic interaction in the framework of the boundary effective theory (BET) formalism. The calculation relies on the solution of the classical equation of motion for the field, and Gaussian fluctuations around it. Our result is non-perturbative and differs from the standard one-loop effective potential for field values larger than .
10 pages, 3 figures
References in corpus (12)
- Generic Rules for High Temperature Dimensional Reduction and Their Application to the Standard Model
- Effective Field Theory Approach to High-Temperature Thermodynamics
- Advances in perturbative thermal field theory
- Resummation in Hot Field Theories
- Screened Perturbation Theory to Three Loops
- Thermodynamics of the high-temperature quark-gluon plasma
- Four-loop screened perturbation theory
- Pressure to order in -theory at weak coupling
- Improved semiclassical density matrix: taming caustics
- Semiclassical thermodynamics of scalar fields
- Quantum statistical correlations in thermal field theories: boundary effective theory
- Pressure of massless hot scalar theory in the boundary effective theory framework