dc.contributor.author |
GANDHI, YATHARTH |
en_US |
dc.contributor.author |
JAIN, SACHIN |
en_US |
dc.contributor.author |
JOHN, RENJAN RAJAN |
en_US |
dc.date.accessioned |
2022-10-21T11:42:55Z |
|
dc.date.available |
2022-10-21T11:42:55Z |
|
dc.date.issued |
2022-08 |
en_US |
dc.identifier.citation |
Physical Review D, 106(4), 046014. |
en_US |
dc.identifier.issn |
2470-0010 |
en_US |
dc.identifier.issn |
2470-0029 |
en_US |
dc.identifier.uri |
https://doi.org/10.1103/PhysRevD.106.046014 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/7412 |
|
dc.description.abstract |
Using a novel relation between the parity-even and -odd parts of a correlator, we show that the three-point function of conserved or weakly broken currents in three-dimensional conformal field theory (CFT) can be obtained from just the free fermion (FF) or the free boson (FB) theory. In the special case of large N Chern-Simons matter theories, we obtain the correlator in terms of a coupling constant dependent “anyonic phase” factor. This anyonic phase factor was previously obtained in the 2→2 exact S-matrix result and is consistent with strong-weak duality. By varying the coupling constant, the CFT correlator interpolates nicely between the same in the FF and FB theories. |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
American Physical Society |
en_US |
dc.subject |
Spins |
en_US |
dc.subject |
2022-OCT-WEEK2 |
en_US |
dc.subject |
TOC-OCT-2022 |
en_US |
dc.subject |
2022 |
en_US |
dc.title |
Anyonic correlation functions in Chern-Simons matter theories |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Physical Review D |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |