Abstract
Two-point functions for interacting quantum fields in statistical systems can be diagnolized by matrix transformations. It is shown, that within the framework of time-dependent Thermo Field Dynamics this diagonalization can be understood as a thermal Bogoliubov transformation to non-interacting statistical quasi-particles. The condition for their unperturbed propagation relates these states to the thermodynamic properties of the system: It requires global equilibrium for stationary situations, or specifies the time evolution according to a kinetic equation. (orig.).
Citation Formats
Henning, P A, and Umezawa, H.
Diagonalization of propagators in thermo field dynamics for relativistic quantum fields.
Germany: N. p.,
1992.
Web.
Henning, P A, & Umezawa, H.
Diagonalization of propagators in thermo field dynamics for relativistic quantum fields.
Germany.
Henning, P A, and Umezawa, H.
1992.
"Diagonalization of propagators in thermo field dynamics for relativistic quantum fields."
Germany.
@misc{etde_10104257,
title = {Diagonalization of propagators in thermo field dynamics for relativistic quantum fields}
author = {Henning, P A, and Umezawa, H}
abstractNote = {Two-point functions for interacting quantum fields in statistical systems can be diagnolized by matrix transformations. It is shown, that within the framework of time-dependent Thermo Field Dynamics this diagonalization can be understood as a thermal Bogoliubov transformation to non-interacting statistical quasi-particles. The condition for their unperturbed propagation relates these states to the thermodynamic properties of the system: It requires global equilibrium for stationary situations, or specifies the time evolution according to a kinetic equation. (orig.).}
place = {Germany}
year = {1992}
month = {Sep}
}
title = {Diagonalization of propagators in thermo field dynamics for relativistic quantum fields}
author = {Henning, P A, and Umezawa, H}
abstractNote = {Two-point functions for interacting quantum fields in statistical systems can be diagnolized by matrix transformations. It is shown, that within the framework of time-dependent Thermo Field Dynamics this diagonalization can be understood as a thermal Bogoliubov transformation to non-interacting statistical quasi-particles. The condition for their unperturbed propagation relates these states to the thermodynamic properties of the system: It requires global equilibrium for stationary situations, or specifies the time evolution according to a kinetic equation. (orig.).}
place = {Germany}
year = {1992}
month = {Sep}
}