2007
DOI: 10.1143/ptp.117.557
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Holography of Two-Point Functions in the Spinning String/Spin Chain Correspondence

Abstract: We study the holographic principle of the two-point function in the case of a spinning string in the AdS/CFT correspondence. Following the general method proposed by Yoneya et al. for the bulk-boundary correspondence in the large J limit, we study the spinning string solution which starts and ends at the boundary. We then show that the spinning string solution directly gives a two-point function that is consistent with the spin chain picture in gauge theory. * )

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Cited by 33 publications
(13 citation statements)
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“…The classical solution for the latter is the Euclidean continuation of the BMN geodesic [41][42][43]:…”
Section: Jhep02(2016)052mentioning
confidence: 99%
“…The classical solution for the latter is the Euclidean continuation of the BMN geodesic [41][42][43]:…”
Section: Jhep02(2016)052mentioning
confidence: 99%
“…They can be obtained by the Euclidean continuation of spinning strings in global AdS. In the Poincaré patch the string worldsheet indeed collapses onto the boundary at two points [16,17,23]. Constructing solutions dual to three-point functions seems to be a difficult problem.…”
Section: Jhep09(2010)030mentioning
confidence: 99%
“…The result obtained this way disagrees with the result calculated in the supergravity approximation [38] when the charges of the two "heavy" BPS states are extrapolated to very large values. This is so because the supergravity approximation is not a priori valid if the charges of the supergravity states 11 By light we mean operators with conformal dimensions ∆ << √ λ.…”
Section: )mentioning
confidence: 99%
“…Recently, another approach to the calculation of n-points correlators involving non-BPS states was developed [11][12][13][14][15]. More precisely, the authors of [12] argued that it should be possible to obtain the correlation functions of local operators corresponding to classical spinning string states, at strong coupling, by evaluating the string action on a classical solution with appropriate boundary conditions after convoluting with the relevant to the classical states wavefunctions.…”
Section: Introductionmentioning
confidence: 99%