Torus conformal blocks and Casimir equations in the necklace channel
A bstract We consider the conformal block decomposition in arbitrary exchange channels of a two-dimensional conformal field theory on a torus. The channels are described by diagrams built of a closed loop with external legs (a necklace sub-diagram) and trivalent vertices forming trivalent trees atta...
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Published in | The journal of high energy physics Vol. 2022; no. 10; pp. 91 - 26 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
14.10.2022
Springer Nature B.V SpringerOpen |
Subjects | |
Online Access | Get full text |
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Summary: | A
bstract
We consider the conformal block decomposition in arbitrary exchange channels of a two-dimensional conformal field theory on a torus. The channels are described by diagrams built of a closed loop with external legs (a necklace sub-diagram) and trivalent vertices forming trivalent trees attached to the necklace. Then, the
n
-point torus conformal block in any channel can be obtained by acting with a number of OPE operators on the
k
-point torus block in the necklace channel at
k
= 1
,
…
, n
. Focusing on the necklace channel, we go to the large-
c
regime, where the Virasoro algebra truncates to the
sl
(2
,
ℝ) subalgebra, and obtain the system of the Casimir equations for the respective
k
-point global conformal block. In the plane limit, when the torus modular parameter
q →
0, we explicitly find the Casimir equations on a plane which define the (
k
+ 2)-point global conformal block in the comb channel. Finally, we formulate the general scheme to find Casimir equations for global torus blocks in arbitrary channels. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP10(2022)091 |