Dissipation in equations of motion of scalar fields
arXiv:hep-ph/0209345 · doi:10.1103/PhysRevD.67.045006
Abstract
The methods of non-equilibrium quantum field theory are used to investigate the possibility of representing dissipation in the equation of motion for the expectation value of a scalar field by a friction term, such as is commonly included in phenomenological inflaton equations of motion. A sequence of approximations is exhibited which reduces the non-equilibrium theory to a set of local evolution equations. However, the adiabatic solution to these evolution equations which is needed to obtain a local equation of motion for the expectation value is not well defined; nor, therefore, is the friction coefficient. Thus, a non-equilibrium treatment is essential, even for a system that remains close to thermal equilibrium, and the formalism developed here provides one means of achieving this numerically.
17 pages, 5 figures
References in corpus (3)
Cited by in corpus (9)
- Warm Inflation and its Microphysical Basis
- Dynamics of Interacting Scalar Fields in Expanding Space-Time
- The warm inflation story
- Fluctuation-dissipation dynamics of cosmological scalar fields
- Thermal effects on slow-roll dynamics
- Spotted Inflation
- Entropy production and curvature perturbation from dissipative curvatons
- Aspects of warm-flat directions
- Numerical investigation of friction in inflaton equations of motion