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M. Guica, “On correlation functions in J T ¯ J\bar{T} -deformed CFTs,” J. Phys
Original
1902
Earlier work this paper cites.
B. Le Floch and M. Mezei, “Solving a family of T T ¯ T\bar{T} -like theories,” arXiv:1903.07606 [hep-th]
Original
1903
Earlier work this paper cites.
R. Conti, S. Negro, and R. Tateo, “Conserved currents and T T ¯ s \text{T}\bar{\text{T}}_{s} irrelevant deformations of 2D integrable field theories,” arXiv:1904.09141 [hep-th]
Original
1904
Earlier work this paper cites.
M. Guica and R. Monten, “ T T ¯ T\bar{T} and the mirage of a bulk cutoff,” arXiv:1906.11251 [hep-th]
Original
1906
Earlier work this paper cites.
J. Cardy, “ T T ¯ T\overline{T} deformation of correlation functions,” arXiv:1907.03394 [hep-th]
Original
1907
Earlier work this paper cites.
L. Apolo and W. Song, “Heating up holography for single-trace J T ¯ J\bar{T} deformations,” arXiv:1907.03745 [hep-th]
Original
1907
Earlier work this paper cites.
J. Aguilera-Damia, V. I. Giraldo-Rivera, E. A. Mazenc, I. Salazar Landea, and R. M. Soni, “A Path Integral Realization of Joint J T ¯ J\bar{T} , T J ¯ T\bar{J} and T T ¯ T\bar{T} Flows,” arXiv:1910.06675 [hep-th]
Original
1910
Earlier work this paper cites.
J. Polchinski, “Evaluation of the One Loop String Path Integral,” Commun. Math. Phys
1986
Earlier work this paper cites.
A. B. Zamolodchikov, “Thermodynamic Bethe Ansatz in Relativistic Models. Scaling Three State Potts and Lee-yang Models,” Nucl. Phys
1990
Earlier work this paper cites.
N. Seiberg and E. Witten, “String theory and noncommutative geometry,” JHEP
1999
Earlier work this paper cites.
A. Bergman and O. J. Ganor, “Dipoles, twists and noncommutative gauge theory,” JHEP
2000
Earlier work this paper cites.

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Then

J. Cardy, “The T T ¯ T\overline{T} deformation of quantum field theory as random geometry,” JHEP
Original
2018
Later among the works it cites.
S. Dubovsky, V. Gorbenko, and G. Hernández-Chifflet, “ T T ¯ T\overline{T} partition function from topological gravity,” JHEP
Original
2018
Later among the works it cites.
L. McGough, M. Mezei, and H. Verlinde, “Moving the CFT into the bulk with T T ¯ T\overline{T} ,” JHEP
Original
2018
Later among the works it cites.
S. Datta and Y. Jiang, “ T T ¯ T\bar{T} deformed partition functions,” JHEP
Original
2018
Later among the works it cites.
M. Guica, “An integrable Lorentz-breaking deformation of two-dimensional CFTs,” SciPost Phys

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2019

A general definition of $JT_a$ -- deformed QFTs

Anous, Tarek, Guica, Monica

Understand

We propose a general path-integral definition of two-dimensional quantum field theories deformed by an integrable, irrelevant vector operator constructed from the components of the stress tensor and those of a $U(1)$ current.

The deformed theory is obtained by coupling the original QFT to a flat dynamical gauge field and "half" a flat dynamical vielbein.
The resulting partition function is shown to satisfy a geometric flow equation, which perfectly reproduces the flow equations for the deformed energy levels that were previously derived in the literature.
The S-matrix of the deformed QFT differs from the original S-matrix only by an overall phase factor that depends on the charges and momenta of the external particles, thus supporting the conjecture that such QFTs are UV complete, although intrinsically non-local.