Abstract
We consider the perturbative construction, proposed in Fredenhagen and Lindner (Commun Math Phys 332:895, 2014), for a thermal state \(\Omega _{\beta ,\lambda V\{f\}}\) for the theory of a real scalar Klein–Gordon field \(\phi \) with interacting potential \(V\{f\}\). Here, f is a space-time cut-off of the interaction V, and \(\lambda \) is a perturbative parameter. We assume that V is quadratic in the field \(\phi \) and we compute the adiabatic limit \(f\rightarrow 1\) of the state \(\Omega _{\beta ,\lambda V\{f\}}\). The limit is shown to exist; moreover, the perturbative series in \(\lambda \) sums up to the thermal state for the corresponding (free) theory with potential V. In addition, we exploit the same methods to address a similar computation for the non-equilibrium steady state (NESS) Ruelle (J Stat Phys 98:57–75, 2000) recently constructed in Drago et al. (Commun Math Phys 357:267, 2018).
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Acknowledgements
The author is grateful to Claudio Dappiaggi, Federico Faldino, Klaus Fredenhagen, Thomas-Paul Hack and Nicola Pinamonti, for enlightening discussions and comments on a preliminary version of this paper. This work was supported by the National Group of Mathematical Physics (GNFMINdAM).
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Communicated by Karl-Henning Rehren.
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Drago, N. Thermal State with Quadratic Interaction. Ann. Henri Poincaré 20, 905–927 (2019). https://doi.org/10.1007/s00023-018-0739-6
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DOI: https://doi.org/10.1007/s00023-018-0739-6