$J\bar T$ - deformed CFTs as non-local CFTs
APA
Guica, M. (2022). $J\bar T$ - deformed CFTs as non-local CFTs . Perimeter Institute. https://pirsa.org/22020055
MLA
Guica, Monica. $J\bar T$ - deformed CFTs as non-local CFTs . Perimeter Institute, Feb. 08, 2022, https://pirsa.org/22020055
BibTex
@misc{ pirsa_PIRSA:22020055, doi = {10.48660/22020055}, url = {https://pirsa.org/22020055}, author = {Guica, Monica}, keywords = {Quantum Fields and Strings}, language = {en}, title = {$J\bar T$ - deformed CFTs as non-local CFTs }, publisher = {Perimeter Institute}, year = {2022}, month = {feb}, note = {PIRSA:22020055 see, \url{https://pirsa.org}} }
TTbar and JTbar - deformed CFTs provide an interesting example of non-local, yet UV-complete two-dimensional QFTs that are entirely solvable. I will start by showing that both classes of theories possess Virasoro x Virasoro or Virasoro- Kac- Moody x Virasoro - Kac- Moody symmetry. For the case of JTbar, I will discuss the classical realization of these symmetries in terms of field-dependent coordinate transformations and show how the associated generators can be used to define an analogue of "primary" operators in this non-local theory, whose correlation functions are entirely fixed in terms of those of the undeformed CFT. In particular, two and three-point functions are simply given by the corresponding momentum-space correlator in the undeformed CFT, with all dimensions replaced by particular momentum-dependent conformal dimensions. Interestingly, scattering amplitudes off the near-horizon of extremal black holes are known to take a strikingly similar form.