2013
DOI: 10.1007/jhep11(2013)081
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Yangian symmetry of smooth Wilson loops in $ \mathcal{N}=4 $ super Yang-Mills theory

Abstract: We show that appropriately supersymmetrized smooth Maldacena-Wilson loop operators in N = 4 super Yang-Mills theory are invariant under a Yangian symmetry Y [psu(2, 2|4)] built upon the manifest superconformal symmetry algebra of the theory. The existence of this hidden symmetry is demonstrated at the one-loop order in the weak coupling limit as well as at leading order in the strong coupling limit employing the classical integrability of the dual AdS 5 × S 5 string description. The hidden symmetry generators … Show more

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Cited by 48 publications
(103 citation statements)
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“…In [34] it was argued that the equivalence holds for any physical solution. With these results in mind, it is likely that one can extend the results of, for example, references [35,36] to the pure spinor string.…”
Section: Conclusion and Prospectsmentioning
confidence: 73%
“…In [34] it was argued that the equivalence holds for any physical solution. With these results in mind, it is likely that one can extend the results of, for example, references [35,36] to the pure spinor string.…”
Section: Conclusion and Prospectsmentioning
confidence: 73%
“…Our focus is on the construction of null polygonal supersymmetric Wilson loops; however, in principle there should be no obstruction to defining a smooth supersymmetric Wilson loop, as done in ref. [13] for N = 4 super Yang-Mills.…”
Section: Jhep06(2014)176mentioning
confidence: 99%
“…The constant can be obtained by using the properties of the Wilson loop under different degenerations. 13 This form can be found for example in ref. [51, eqs.…”
Section: Some Perturbative Computationsmentioning
confidence: 99%
“…There is a large amount of work on the subject, see for example [6][7][8][9][10] and, in particular [11][12][13][14][15][16][17][18][19][20] for the circular Wilson loop, the most studied case. The main interest of this problem is its integrability properties [21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36]. The basic idea is that the computation of the Wilson loops in the strong coupling limit is translated into finding the area of the minimal surface ending on a boundary curve defined by the Wilson loop.…”
Section: Introductionmentioning
confidence: 99%