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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Published in | Chinese physics C Vol. 34; no. 9; pp. 1355 - 1359 |
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Main Author | |
Format | Journal Article |
Language | English |
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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Online Access | Get full text |
ISSN | 1674-1137 0254-3052 2058-6132 |
DOI | 10.1088/1674-1137/34/9/041 |
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Abstract | 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. |
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AbstractList | 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. O4; Applying the AdS/CFT correspondence,the expansion of the heavy-quark potential of N= 4supersymmetric Yang-Mills theory at large Nc 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. |
Author | 初少霞 侯德富 任海沧 |
AuthorAffiliation | 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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Cites_doi | 10.1103/PhysRevD.69.046005 10.1088/1126-6708/2002/06/007 10.1088/1126-6708/2000/04/021 10.1103/PhysRevD.80.046007 10.4310/ATMP.1998.v2.n2.a1 10.1016/S0550-3213(98)00471-4 10.1103/PhysRevLett.80.4859 10.1088/1126-6708/1999/08/013 10.1103/PhysRevLett.97.182301 10.1103/PhysRevLett.87.081601 10.1088/1126-6708/2008/05/064 10.1016/S0370-2693(98)00377-3 10.1103/PhysRevD.77.021701 10.4310/ATMP.1998.v2.n2.a2 10.1023/A:1026654312961 10.1016/S0550-3213(98)00570-7 10.1016/j.nuclphysb.2004.11.055 10.1088/1126-6708/1998/09/010 10.1016/S0550-3213(98)00514-8 10.1016/S0370-1573(99)00083-6 10.1016/S0550-3213(00)00300-X |
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Snippet | 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... O4; Applying the AdS/CFT correspondence,the expansion of the heavy-quark potential of N= 4supersymmetric Yang-Mills theory at large Nc is carried out to the... |
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Title | On the Next-leading order Heavy-Quark Potential from AdS/CFT |
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