# conformal dimension of an operator

Consider a general coordinate transformation x!x0, such that x = f (x0 ). High Energy Phys. one inevitably must come to an operator for which the addendum O α μ on the r.h.s. Since the scaling dimension of the operator O α μ is less than that of O Δ α by one, applying the conformal transformations subsequently to O Δ α, O α μ etc. 1.1.3 Conformal invariance A conformal transformation can now be de ned as a coordinate transformation which acts on the metric as a Weyl transformation. Featured on Meta Creating new Help Center documents for Review queues: Project overview Browse other questions tagged lie-algebras conformal-field-theory kac-moody-algebras or ask your own question. The four-point conformal block plays an important part in the analysis of the conformally invariant operator algebra in two-dimensional space. Conformal field theory, tensor categories and ... where the space and the time are mixed into one dimension. Abstract. 2. The behavior of the conformal block is calculated in the present paper in the limit in which the dimension A of the intermediate operator tends to infinity. We continue the study of model-independent constraints on the unitary conformal field theories (CFTs) in four dimensions, initiated in [R. Rattazzi, V. S. Rychkov, E. Tonni, and A. Vichi, J. 12 (2008) 031]. The bound we find is of the same form as found by Hellerman for ∆ 1: ∆ 2 ≤ + O(1). an operator that transforms homogeneously under conformal transformations. We further com- ... and [130] for a recent review on the operator algebraic approach to conformal ﬁeld theory. vanishes, i.e. This has the following e ect on the metric g (x) !g0 (x 0) = @fˆ @x 0 @f˙ @x g ˆ˙(f(x0)) : (1.8) Basics of operator algebras We prepare basic facts about operator algebras which are necessary for studying conformal We extend the work of Hellerman [1] to derive an upper bound on the conformal dimension ∆ 2 of the next-to-lowest nontrival primary operator in unitary, modular-invariant two-dimensional conformal field theories without chiral primary operators, with total central charge c tot > 2.

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