2016
DOI: 10.1007/jhep06(2016)119
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Holographic conformal partial waves as gravitational open Wilson networks

Abstract: We propose a method to holographically compute the conformal partial waves in any decomposition of correlation functions of primary operators in conformal field theories using open Wilson network operators in the holographic gravitational dual. The Wilson operators are the gravitational ones where gravity is written as a gauge theory in the first order Hilbert-Palatini formalism. We apply this method to compute the global conformal blocks and partial waves in 2d CFTs reproducing many of the known results.

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Cited by 49 publications
(94 citation statements)
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“…where β ∞ (·, ·) is defined in (11). Note that setting k 1 = k 2 = k 3 = 0 in (22) recovers the p-adic form of the geodesic bulk diagram given in figure 4.…”
Section: Holographic Dual Of the Five-point Conformal Blockmentioning
confidence: 88%
See 1 more Smart Citation
“…where β ∞ (·, ·) is defined in (11). Note that setting k 1 = k 2 = k 3 = 0 in (22) recovers the p-adic form of the geodesic bulk diagram given in figure 4.…”
Section: Holographic Dual Of the Five-point Conformal Blockmentioning
confidence: 88%
“…Such a task was recently undertaken for four-point global conformal blocks in any dimension with external scalar operators [1] (with further generalizations in Refs. [2,3,4,5,6,7,8,9,10,11,12,13]) and for Virasoro blocks in AdS 3 /CFT 2 [14,15,16,17,18,19,20,21,22,23,24].…”
Section: Introductionmentioning
confidence: 99%
“…In this section we recall the basic construction of the Wilson line, and how it provides a representation of Virasoro conformal blocks that admits a convenient expansion at large central charge. See [8][9][10][11][12][13][14][15] for more background and previous results.…”
Section: The Virasoro Wilson Linementioning
confidence: 99%
“…For a numerical study, see [7]. Our approach is via the Wilson representation of conformal blocks, as developed in [8][9][10][11][12][13][14][15]. Here, the conformal block corresponding to OO → stress tensors → O O is expressed as h, h |P e z 2 z 1 (L 1 + 6 c T (z)L 1 )dz |h, h , where T (z) is the CFT stress tensor.…”
Section: Introductionmentioning
confidence: 99%
“…Simons formulation [33,34], for recent discussion see, e.g., [35][36][37][38]. Finally, it is interesting to develop the geodesic Witten diagrams technique by analogy with conformal blocks on the complex plane [10].…”
Section: Jhep06(2016)183mentioning
confidence: 99%