Ope between the Energy-momentum Tensor and the Wilson Loop in N = 4 Super-yang-mills Theory Typeset Using Ptpt E X.sty <ver.1.0> 2
نویسنده
چکیده
Conformal field theory (CFT) is important in modern particle physics in various contexts. The most powerful tool in the 2-dimensional CFT is the operator product expansion (OPE). The OPE between the energy-momentum tensor and an operator extracts its conformal weight. We find it interesting to consider the similar issue with respect to the Wilson loop in a conformally invariant Yang-Mills theory. We investigate the OPE between the energy-momentum tensor and the Wilson loop in N = 4 4-dimensional Super-YangMills (SYM) theory with U(N) gauge group by means of the dimensional analysis and the properties of the energy-momentum tensor. We clarify that the Wilson loop in N = 4 SYM theory does not possess an anomalous dimension and that only the deformation of the loop occurs under the conformal transformation. Another interesting issue is the AdS/CFT correspondence 1). The AdS/CFT correspondence enables one to evaluate such physical quantities as the multi-point function 4) and the expectation value of the Wilson loop 2) 3) in strong coupling region. Yet, there have been ambitious attempts to compute the expectation value of the Wilson loop in strong coupling region by means of the quantum field theory 6) 7) for a direct test of AdS/CFT correspondence. Especially, Gross and Drukker 7) pointed out that the expectation value of the circular Wilson loop in N = 4 4-dimensional SYM theory is determined by an anomaly in the conformal transformation that relates the circular loop to the straight line, and computed the expectation value of the circular Wilson loop to all orders in the 1 N2 expansion. However, their analysis is based on the Feynman gauge, and the generalization to the general gauge is nontrivial. We attempt to grasp the conformal anomaly via the OPE between the energy-momentum tensor and the closed Wilson loop, taking advantage of its gauge invariance. This paper is organized as follows. Sec. 2. is devoted to the OPE between
منابع مشابه
OPE between the energy - momentum tensor and the Wilson loop in N = 4 Super - Yang - Mills theory
We analyze the operator product expansion Tμν(z)W [C] in N = 4 4-dimensional Super-Yang-Mills(SYM) theory with U(N) gauge group, and clarify that the closed Wilson loop does not possess an anomalous dimension and that only the shape of the loop is changed by the conformal transformation.
متن کامل3 - Point Functions in N = 4 Yang - Mills
Three-point functions of analytic (chiral primary) operators in N = 4 Yang-Mills theory in four dimensions are calculated using the harmonic superspace formulation of this theory. In the case of the energy-momentum tensor multiplet anomaly considerations determine the coefficient. Analyticity in N = 2 harmonic superspace is explicitly checked in a two-loop calculation.
متن کاملWilson loop correlators at strong coupling: from matrices to bubbling geometries
We compute at strong coupling the largeN correlation functions of supersymmetric Wilson loops in large representations of the gauge group with local operators of N = 4 super Yang-Mills. The gauge theory computation of these correlators is performed using matrix model techniques. We show that the strong coupling correlator of the Wilson loop with the stress tensor computed using the matrix model...
متن کاملGluon scattering in N = 4 Super Yang-Mills at finite temperature
We extend the AdS/CFT prescription of Alday and Maldacena to finite temperature T , defining an amplitude for gluon scattering in N = 4 Super Yang-Mills at strong coupling from string theory. It is defined by a lightlike ”Wilson loop” living at the horizon of the T-dual to the black hole in AdS space. Unlike the zero temperature case, this is different from the Wilson loop contour defined at th...
متن کاملThe N=4 Quantum Conformal Algebra
We determine the spectrum of currents generated by the operator product expansion of the energy-momentum tensor in N=4 super-symmetric Yang-Mills theory. Up to the regular terms and in addition to the multiplet of the stress tensor, three current multiplets appear, Σ, Ξ and Υ, starting with spin 0, 2 and 4, respectively. The OPE’s of these new currents generate an infinite tower of current mult...
متن کامل