Quasiparticles in Finite-Temperature Field Theory

Physics – High Energy Physics – High Energy Physics - Phenomenology

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

10 pages, RevTex twocolumn; small improvements in text and references

Scientific paper

Conventional finite-temperature perturbation theory in which propagators have poles at $k^{2}=m^{2}$ is shown to break down at the two-loop level for self-interacting scalar fields. The breakdown is avoided by using free thermal propagators that have poles at the same energy as the exact thermal propagator. This quasiparticle energy ${\cal E}(\vec{k})$ is temperature-dependent, complex, and gauge invariant. An operator theory containing two self-adjoint scalar fields is presented in which all temperature dependence is incorporated into the Hamiltonian. No thermal traces are required to compute thermal Green functions. Choosing the spectrum of the unperturbed part of the Hamiltonian to contain the exact quasiparticle energy ${\cal E}(\vec{k})$ produces a resummed perturbation theory that has the correct poles and branch cuts. The location of the poles and cuts is explained directly in terms of the spectrum of the Hamiltonian.

No associations

LandOfFree

Say what you really think

Search LandOfFree.com for scientists and scientific papers. Rate them and share your experience with other people.

Rating

Quasiparticles in Finite-Temperature Field Theory does not yet have a rating. At this time, there are no reviews or comments for this scientific paper.

If you have personal experience with Quasiparticles in Finite-Temperature Field Theory, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Quasiparticles in Finite-Temperature Field Theory will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-718954

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.