The thermal operator representation for Matsubara sums
arXiv:hep-ph/0501273 · doi:10.1103/PhysRevD.71.065009
Abstract
We prove in full generality the thermal operator representation for Matsubara sums in a relativistic field theory of scalar and fermionic particles. It states that the full result of performing the Matsubara sum associated to any given Feynman graph, in the imaginary-time formalism of finite-temperature field theory, can be directly obtained from its corresponding zero-temperature energy integral, by means of a simple linear operator, which is independent of the external Euclidean energies and whose form depends solely on the topology of the graph.
9 pages, 1 figure, RevTex
References in corpus (3)
Cited by in corpus (12)
- Shear viscosity of quark matter at finite temperature in magnetic fields
- Isolating vacuum amplitudes in quantum field calculations at finite temperature
- Thermal Operator Representation of Finite Temperature Graphs
- Hard Thermal Loop -- theory and applications
- Thermal Operator Representation of Finite Temperature Graphs II
- Factorization of finite temperature graphs in thermal QED
- Forward scattering amplitudes and the thermal operator representation
- Thermal Operator Representation of Finite-Temperature Amplitudes in the Presence of Chemical Potential
- Thermal Operator and Cutting Rules at Finite Temperature and Chemical Potential
- Hard thermal effective action in QCD through the thermal operator
- Thermal Operator and Dispersion Relation in QED at Finite Temperature and Chemical Potential
- On the evaluation of Matsubara sums