Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:hep-th/9909019 · Nuclear Physics B

A comment on finite temperature correlations in integrable QFT

Hubert Saleur

Published Feb 1, 2000• 114 citations
arXivHTMLPDF
DOI
10.1016/s0550-3213(99)00665-3

Related papers

Finite temperature correlation functions in integrable QFT

André LeClair, G. Mussardo

Finite temperature correlation functions in integrable quantum field theories are formulated only in terms of the usual, temperature-independent form factors, and certain thermodynamic filling fractions which are determined from the thermodynamic Bethe ansatz. Explicit expressions are given for the one- and two-point functions.

arXiv:hep-th/9902075•Nuclear Physics B•Jul 1, 1999•160 citations

Correlation functions in integrable quantum field theory

Benjamin Doyon

•Jan 1, 2004•3 citations

The integrable SU(N) Heisenberg model at finite temperature

Henrik Johannesson

Physics Letters A•Jun 1, 1986•35 citations

Finite Temperature Correlation Functions in Integrable QFT

André LeClair, Giuseppe Mussardo

Finite temperature correlation functions in integrable quantum field theories are formulated only in terms of the usual, temperature-independent form factors, and certain thermodynamic filling fractions which are determined from the thermodynamic Bethe ansatz. Explicit expressions are given for the one and two-point functions. Typeset using REVTEX 1 I.

•Jan 1, 1999•97 citations

Two-point correlation function in integrable QFT with anti-crossing symmetry

G. Delfino, G. Mussardo

arXiv:hep-th/9310130•Physics Letters B•Mar 1, 1994•37 citations

Comment on "Dual path integral representation for finite temperature quantum field theory"

Peter O. Kazinski

I show that the novel dual path integral representation for finite temperature quantum field theory proposed in [Phys. Rev. D 77, 105030 (2008), arXiv:0803.1667 ] is a well-known representation of quantum mechanics in terms of symbols of operators.

arXiv:0809.1794•Sep 10, 2008•0 citations