On the Next-leading order Heavy-Quark Potential from AdS/CFT

Applying the AdS/CFT correspondence,the expansion of the heavy-quark potential of N = 4 supersymmetric Yang-Mills theory at large N c is carried out to the next-leading term in the large ’t Hooft coupling at zero temperature.The strong coupling corresponds to the semi-classical expansion of the stri...

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Bibliographic Details
Published inChinese physics C Vol. 34; no. 9; pp. 1355 - 1359
Main Author 初少霞 侯德富 任海沧
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.09.2010
Institute of Particle Physics,Huazhong Normal University,Wuhan 430079,China%Physics Department,The Rockefeller University,1230 York Avenue,New York,NY 10021-6399,USA
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ISSN1674-1137
0254-3052
2058-6132
DOI10.1088/1674-1137/34/9/041

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Summary:Applying the AdS/CFT correspondence,the expansion of the heavy-quark potential of N = 4 supersymmetric Yang-Mills theory at large N c is carried out to the next-leading term in the large ’t Hooft coupling at zero temperature.The strong coupling corresponds to the semi-classical expansion of the stringsigma model,the gravity dual of the Wilson loop operator,with the next-leading term expressed in terms of functional determinants of fluctuations.The singularities of these determinants are examined and their contributions are evaluated numerically.We find the next-leading order correction is negative and suppressed by minus square root of the ’t Hooft coupling relative to the leading order.
Bibliography:11-5641/O4
heavy quarkonium
D815.5
holographic QCD; heavy quarkonium
holographic QCD
O572.33
ISSN:1674-1137
0254-3052
2058-6132
DOI:10.1088/1674-1137/34/9/041