We use the AdS/CFT correspondence to calculate three point functions of chiral primary operators at large N in d = 3, N = 8 and d=6, N = (2,0) superconformal field theories. These theories are related to the infrared fixed points of world-volume descriptions of N coincident M2 and M5 branes, respectively. The computation can be generalized by employing a gravitational action in arbitrary dimensions D, coupled to a (p + 1)-form and appropriately compactified on AdS(D-p-2) × S(p + 2). We note a surprising coincidence: this generalized model reproduces for D = 10, p = 3 the three point functions of d = 4, N = 4 SYM chiral primary operators at large N. © 1999 Published by Elsevier Science B.V. All rights reserved.
Bastianelli F., Zucchini R. (1999). Three point functions of chiral primary operators in d= 3, N = 8 and d=6, N = (2,0) SCFT at large N. PHYSICS LETTERS. SECTION B, 467(1-2), 61-66 [10.1016/S0370-2693(99)01179-X].
Three point functions of chiral primary operators in d= 3, N = 8 and d=6, N = (2,0) SCFT at large N
Bastianelli F.;Zucchini R.
1999
Abstract
We use the AdS/CFT correspondence to calculate three point functions of chiral primary operators at large N in d = 3, N = 8 and d=6, N = (2,0) superconformal field theories. These theories are related to the infrared fixed points of world-volume descriptions of N coincident M2 and M5 branes, respectively. The computation can be generalized by employing a gravitational action in arbitrary dimensions D, coupled to a (p + 1)-form and appropriately compactified on AdS(D-p-2) × S(p + 2). We note a surprising coincidence: this generalized model reproduces for D = 10, p = 3 the three point functions of d = 4, N = 4 SYM chiral primary operators at large N. © 1999 Published by Elsevier Science B.V. All rights reserved.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
