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最大超对称杨-米尔斯理论中的平面振幅

Planar amplitudes in maximally supersymmetric Yang-Mills theory.

作者信息

Anastasiou C, Dixon L, Bern Z, Kosower D A

机构信息

Stanford Linear Accelerator Center, Stanford University, Stanford, California 94309, USA.

出版信息

Phys Rev Lett. 2003 Dec 19;91(25):251602. doi: 10.1103/PhysRevLett.91.251602. Epub 2003 Dec 18.

Abstract

The collinear factorization properties of two-loop scattering amplitudes in dimensionally regulated N=4 super-Yang-Mills theory suggest that, in the planar ('t Hooft) limit, higher-loop contributions can be expressed entirely in terms of one-loop amplitudes. We demonstrate this relation explicitly for the two-loop four-point amplitude and, based on the collinear limits, conjecture an analogous relation for n-point amplitudes. The simplicity of the relation is consistent with intuition based on the anti-de Sitter/conformal field theory correspondence that the form of the large-N(c) L-loop amplitudes should be simple enough to allow a resummation to all orders.

摘要

在维数正规化的(N = 4)超杨-米尔斯理论中,两圈散射振幅的共线因子分解性质表明,在平面('t Hooft)极限下,更高圈的贡献可以完全用一圈振幅来表示。我们明确地证明了两圈四点振幅的这种关系,并基于共线极限,推测了(n)点振幅的类似关系。该关系的简单性与基于反德西特/共形场理论对应关系的直觉一致,即大(N_c) (L)圈振幅的形式应该足够简单,以便能够对所有阶次进行求和。

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