Holographic variables for CFT2 conformal blocks with heavy operators

We consider large-c n-point Virasoro blocks with n−k background heavy operators and k perturbative heavy operators. Conformal dimensions of heavy operators scale linearly with large c, while splitting into background/perturbative operators assumes an additional perturbative expansion. Such conformal...

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Main Authors: Konstantin Alkalaev, Mikhail Pavlov
Format: Article
Language:English
Published: Elsevier 2020-07-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321320301048
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spelling doaj-337c0b5dbc704523a8540fd82f3e810e2020-11-25T03:09:29ZengElsevierNuclear Physics B0550-32132020-07-01956115018Holographic variables for CFT2 conformal blocks with heavy operatorsKonstantin Alkalaev0Mikhail Pavlov1I.E. Tamm Department of Theoretical Physics, P.N. Lebedev Physical Institute, Leninsky ave. 53, 119991 Moscow, Russia; Department of General and Applied Physics, Moscow Institute of Physics and Technology, Institutskiy per. 7, Dolgoprudnyi, 141700 Moscow region, RussiaI.E. Tamm Department of Theoretical Physics, P.N. Lebedev Physical Institute, Leninsky ave. 53, 119991 Moscow, RussiaWe consider large-c n-point Virasoro blocks with n−k background heavy operators and k perturbative heavy operators. Conformal dimensions of heavy operators scale linearly with large c, while splitting into background/perturbative operators assumes an additional perturbative expansion. Such conformal blocks can be calculated within the monodromy method that basically reduces to solving auxiliary Fuchsian second-order equation and finding monodromy of solutions. We show that there exist particular variables that we call holographic, use of which drastically simplifies the whole analysis. In consequence, we formulate the uniformization property of the large-c blocks which states that in the holographic variables their form depends only on the number of perturbative heavy operators. On the other hand, the holographic variables encode the metric in the bulk space so that the conformal blocks with the same number of perturbative operators are calculated by the same geodesic trees but on different geometries created by the background operators.http://www.sciencedirect.com/science/article/pii/S0550321320301048
collection DOAJ
language English
format Article
sources DOAJ
author Konstantin Alkalaev
Mikhail Pavlov
spellingShingle Konstantin Alkalaev
Mikhail Pavlov
Holographic variables for CFT2 conformal blocks with heavy operators
Nuclear Physics B
author_facet Konstantin Alkalaev
Mikhail Pavlov
author_sort Konstantin Alkalaev
title Holographic variables for CFT2 conformal blocks with heavy operators
title_short Holographic variables for CFT2 conformal blocks with heavy operators
title_full Holographic variables for CFT2 conformal blocks with heavy operators
title_fullStr Holographic variables for CFT2 conformal blocks with heavy operators
title_full_unstemmed Holographic variables for CFT2 conformal blocks with heavy operators
title_sort holographic variables for cft2 conformal blocks with heavy operators
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2020-07-01
description We consider large-c n-point Virasoro blocks with n−k background heavy operators and k perturbative heavy operators. Conformal dimensions of heavy operators scale linearly with large c, while splitting into background/perturbative operators assumes an additional perturbative expansion. Such conformal blocks can be calculated within the monodromy method that basically reduces to solving auxiliary Fuchsian second-order equation and finding monodromy of solutions. We show that there exist particular variables that we call holographic, use of which drastically simplifies the whole analysis. In consequence, we formulate the uniformization property of the large-c blocks which states that in the holographic variables their form depends only on the number of perturbative heavy operators. On the other hand, the holographic variables encode the metric in the bulk space so that the conformal blocks with the same number of perturbative operators are calculated by the same geodesic trees but on different geometries created by the background operators.
url http://www.sciencedirect.com/science/article/pii/S0550321320301048
work_keys_str_mv AT konstantinalkalaev holographicvariablesforcft2conformalblockswithheavyoperators
AT mikhailpavlov holographicvariablesforcft2conformalblockswithheavyoperators
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