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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2020-07-01
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Series: | Nuclear Physics B |
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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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1724662416325738496 |