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DC Field | Value | Language |
---|---|---|
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 |
Appears in Collections: | JOURNAL ARTICLES |
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