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Constructing the correlation function of four stress-tensor multiplets and the four-particle amplitude in N=4 SYM

机译:在N = 4 SYM下构造四个应力张量多重峰与四个粒子振幅的相关函数

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We present a construction of the integrand of the correlation function of four stress-tensor multiplets in. N=4 SYM at weak coupling. It does not rely on Feynman diagrams and makes use of the recently discovered symmetry of the integrand under permutations of external and integration points. This symmetry holds for any gauge group, so it can be used to predict the integrand both in the planar and non-planar sectors. We demonstrate the great efficiency of graph-theoretical tools in the systematic study of the possible permutation symmetric integrands. We formulate a general ansatz for the correlation function as a linear combination of all relevant graph topologies, with arbitrary coefficients. Powerful restrictions on the coefficients come from the analysis of the logarithmic divergences of the correlation function in two singular regimes: Euclidean short-distance and Minkowski light-cone limits. We demonstrate that the planar integrand is completely fixed by the procedure up to six loops and probably beyond. In the non-planar sector, we show the absence of non-planar corrections at three loops and we reduce the freedom at four loops to just four constants. Finally, the correlation function/amplitude duality allows us to show the complete agreement of our results with the four-particle planar amplitude in. N=4 SYM.
机译:我们提出了在弱耦合条件下,N = 4 SYM中四个应力张量多重态的相关函数的被积的构造。它不依赖于费曼图,而是利用了最近发现的在外部和积分点置换下被积物的对称性。这种对称性适用于任何量规组,因此可以用来预测平面和非平面扇区中的积分。我们在系统研究可能排列对称被积数的过程中证明了图论工具的巨大效率。我们将相关函数的通用ansatz公式化为所有相关图拓扑的线性组合,具有任意系数。对系数的强大限制来自对两种奇异状态下相关函数对数散度的分析:欧几里得短距离和明可夫斯基光锥极限。我们证明平面积分被程序最多完全固定,最多六个循环,甚至可能更多。在非平面扇区中,我们显示了在三个循环中没有非平面校正,并且我们将四个循环中的自由度减小到只有四个常数。最后,相关函数/振幅对偶性使我们能够证明我们的结果与N = 4 SYM处的四粒子平面振幅完全吻合。

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