Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve

Abstract We continue our study of large charge limits of the defect CFT defined by the half-BPS Wilson loop in planar N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory. In this paper, we compute 1/J corrections to the correlation function of two heavy insertions of charge J and two light inse...

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Main Authors: Simone Giombi, Shota Komatsu, Bendeguz Offertaler
Format: Article
Language:English
Published: SpringerOpen 2022-08-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP08(2022)011
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author Simone Giombi
Shota Komatsu
Bendeguz Offertaler
author_facet Simone Giombi
Shota Komatsu
Bendeguz Offertaler
author_sort Simone Giombi
collection DOAJ
description Abstract We continue our study of large charge limits of the defect CFT defined by the half-BPS Wilson loop in planar N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory. In this paper, we compute 1/J corrections to the correlation function of two heavy insertions of charge J and two light insertions, in the double scaling limit where the charge J and the ’t Hooft coupling λ are sent to infinity with the ratio J/ λ $$ \sqrt{\lambda } $$ fixed. Holographically, they correspond to quantum fluctuations around a classical string solution with large angular momentum, and can be computed by evaluating Green’s functions on the worldsheet. We derive a representation of the Green’s functions in terms of a sum over residues in the complexified Fourier space, and show that it gives rise to the conformal block expansion in the heavy-light channel. This allows us to extract the scaling dimensions and structure constants for an infinite tower of non-protected dCFT operators. We also find a close connection between our results and the semi-classical integrability of the string sigma model. The series of poles of the Green’s functions in Fourier space corresponds to points on the spectral curve where the so-called quasi-momentum satisfies a quantization condition, and both the scaling dimensions and the structure constants in the heavy-light channel take simple forms when written in terms of the spectral curve. These observations suggest extensions of the results by Gromov, Schafer-Nameki and Vieira on the semiclassical energy of closed strings, and in particular hint at the possibility of determining the structure constants directly from the spectral curve.
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spelling doaj.art-f6e7006f68df44c3a2c89a1f2b1a258c2022-12-22T02:33:37ZengSpringerOpenJournal of High Energy Physics1029-84792022-08-012022819110.1007/JHEP08(2022)011Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curveSimone Giombi0Shota Komatsu1Bendeguz Offertaler2Joseph Henry Laboratories, Princeton UniversityDepartment of Theoretical Physics, CERNJoseph Henry Laboratories, Princeton UniversityAbstract We continue our study of large charge limits of the defect CFT defined by the half-BPS Wilson loop in planar N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory. In this paper, we compute 1/J corrections to the correlation function of two heavy insertions of charge J and two light insertions, in the double scaling limit where the charge J and the ’t Hooft coupling λ are sent to infinity with the ratio J/ λ $$ \sqrt{\lambda } $$ fixed. Holographically, they correspond to quantum fluctuations around a classical string solution with large angular momentum, and can be computed by evaluating Green’s functions on the worldsheet. We derive a representation of the Green’s functions in terms of a sum over residues in the complexified Fourier space, and show that it gives rise to the conformal block expansion in the heavy-light channel. This allows us to extract the scaling dimensions and structure constants for an infinite tower of non-protected dCFT operators. We also find a close connection between our results and the semi-classical integrability of the string sigma model. The series of poles of the Green’s functions in Fourier space corresponds to points on the spectral curve where the so-called quasi-momentum satisfies a quantization condition, and both the scaling dimensions and the structure constants in the heavy-light channel take simple forms when written in terms of the spectral curve. These observations suggest extensions of the results by Gromov, Schafer-Nameki and Vieira on the semiclassical energy of closed strings, and in particular hint at the possibility of determining the structure constants directly from the spectral curve.https://doi.org/10.1007/JHEP08(2022)011AdS-CFT CorrespondenceWilson, ’t Hooft and Polyakov loops
spellingShingle Simone Giombi
Shota Komatsu
Bendeguz Offertaler
Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve
Journal of High Energy Physics
AdS-CFT Correspondence
Wilson, ’t Hooft and Polyakov loops
title Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve
title_full Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve
title_fullStr Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve
title_full_unstemmed Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve
title_short Large charges on the Wilson loop in N $$ \mathcal{N} $$ = 4 SYM. Part II. Quantum fluctuations, OPE, and spectral curve
title_sort large charges on the wilson loop in n mathcal n 4 sym part ii quantum fluctuations ope and spectral curve
topic AdS-CFT Correspondence
Wilson, ’t Hooft and Polyakov loops
url https://doi.org/10.1007/JHEP08(2022)011
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AT bendeguzoffertaler largechargesonthewilsonloopinnmathcaln4sympartiiquantumfluctuationsopeandspectralcurve