The full four-loop cusp anomalous dimension in N = 4 super Yang-Mills and QCD
A bstract We present the complete formula for the cusp anomalous dimension at four loops in QCD and in maximally supersymmetric Yang-Mills. In the latter theory it is given by Γ cusp , A α s 4 = − α s N π 4 73 π 6 20160 + ζ 3 2 8 + 1 N 2 31 π 6 5040 + 9 ζ 3 2 4 . Our approach is based on computing t...
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Published in | The journal of high energy physics Vol. 2020; no. 4 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
03.04.2020
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | A
bstract
We present the complete formula for the cusp anomalous dimension at four loops in QCD and in maximally supersymmetric Yang-Mills. In the latter theory it is given by
Γ
cusp
,
A
α
s
4
=
−
α
s
N
π
4
73
π
6
20160
+
ζ
3
2
8
+
1
N
2
31
π
6
5040
+
9
ζ
3
2
4
.
Our approach is based on computing the correlation function of a rectangular light-like Wilson loop with a Lagrangian insertion, normalized by the expectation value of the Wilson loop. In maximally supersymmetric Yang-Mills theory, this ratio is a finite function of a cross-ratio and the coupling constant. We compute it to three loops, including the full colour dependence. Integrating over the position of the Lagrangian insertion gives the four-loop Wilson loop. We extract its leading divergence, which determines the four-loop cusp anomalous dimension. Finally, we employ a supersymmetric decomposition to derive the last missing ingredient in the corresponding QCD result. |
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ISSN: | 1029-8479 |
DOI: | 10.1007/JHEP04(2020)018 |