Three-point correlators of stress tensors in maximally-supersymmetric conformal theories in d=3 and d=6

被引:36
作者
Bastianelli, F
Frolov, S
Tseytlin, AA
机构
[1] Ist Nazl Fis Nucl, Sezione Bologna, I-40126 Bologna, Italy
[2] Ist Nazl Fis Nucl, Dipartimento Fis, I-40126 Bologna, Italy
[3] Univ Alabama, Dept Phys & Astron, Tuscaloosa, AL 35487 USA
[4] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
[5] Steklov Math Inst, Moscow, Russia
[6] Univ London Imperial Coll Sci Technol & Med, London, England
[7] Lebedev Phys Inst, Moscow, Russia
关键词
D O I
10.1016/S0550-3213(99)00822-6
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We consider free superconformal theories of N = 8 scalar multiplet in d = 3 and (2, 0) tensor multiplet in d = 6 and compute 2-point and 3-point correlators of their stress tensors. The results for the 2-point and the 3-point correlators for a single d = 3 and d = 6 multiplet differ from 4 root 2/3 pi N-3/2 and 4N(3) the "strong-coupling" AdS(4) and AdS(7) supergravity predictions by the factors respectively These are the same factors as found earlier in hep-th/9703040 in the comparison of the brane free field theory and the d = 11 supergravity predictions for the absorption cross sections of longitudinally polarized gravitons by N M2 and M5 branes. While the correspondence of the results for the cross sections and 2-point functions was expected on the basis of unitarity, the fact that the same coefficients appear in the ratio of the free-theory and supergravity 3-point functions is nontrivial. Thus, like in the d = 4 SYM case, in both d = 3 and d = 6 theories the ratio of the 3-point and 2-point correlators (TTT)/(TT) is exactly the same in the free field theory and in the interacting CFT as described (to leading order in large N) by the Ii-dimensional supergravity on AdS(d+1) x S10-d. (C) 2000 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:139 / 152
页数:14
相关论文
共 59 条
[1]   M theory on AdSpxS11-p and superconformal field theories [J].
Aharony, O ;
Oz, Y ;
Yin, Z .
PHYSICS LETTERS B, 1998, 430 (1-2) :87-93
[2]  
Aharony O., 1998, ADV THEOR MATH PHYS, V1, P148, DOI DOI 10.4310/ATMP.1997.V1.N1.A5
[3]  
AHARONY O, HEPTH9712117
[4]  
Aharony O., 1998, ADV THEOR MATH PHYS, V2, P119, DOI [10.4310/ATMP.1998.v2.n1.a5[hep-th/9712117, DOI 10.4310/ATMP.1998.V2.N1.A5]
[5]  
AHARONY O, HEPTH9905111
[6]   GRAVITATIONAL ANOMALIES [J].
ALVAREZGAUME, L ;
WITTEN, E .
NUCLEAR PHYSICS B, 1984, 234 (02) :269-330
[7]  
ANSELMI D, HEPTH9906167
[8]   Three-point Green function of the stress-energy tensor in the AdS-CFT correspondence [J].
Arutyunov, G ;
Frolov, S .
PHYSICAL REVIEW D, 1999, 60 (02)
[9]  
Awata H, 1999, ADV THEOR MATH PHYS, V3, P147, DOI 10.4310/ATMP.1999.v3.n1.a6
[10]   Non-perturbative effects in AdS5xS5 string theory and d=4 SUSY Yang-Mills [J].
Banks, T ;
Green, MB .
JOURNAL OF HIGH ENERGY PHYSICS, 1998, (05) :XII-15