Abstract

We give evidence that spacelike BPS Wilson loops do not exist in Minkowski spacetime. We show that spacelike Wilson loops in Minkowski spacetime cannot preserve any supersymmetries, in $$d = 4$$ $$\mathcal N = 4$$ super Yang–Mills theory, $$d = 3$$ $$\mathcal N = 2$$ super Chern–Simons-matter theory, and $$d = 3$$ $$\mathcal N = 6$$ Aharony–Bergman–Jafferis–Maldacena theory. We not only show this using infinite straight lines and circles as examples, but also we give proofs for general curves. We attribute this to the conflicts of the reality conditions of the spinors. However, spacelike Wilson loops do exist in Euclidean space. There are both BPS Wilson loops along infinite straight lines and circular BPS Wilson loops. This is because the reality conditions of the spinors are lost after Wick rotation. The result is reasonable in view of the AdS/CFT correspondence.

Highlights

  • In this paper we revisit the Wilson loops in the AdS/CFT correspondence

  • The reality conditions of the spinors are lost in the Wick rotation, and the conflicts in Minkowski spacetime disappear in Euclidean space

  • We have discussed BPS Wilson loops in several superconformal theories, namely the d = 4 N = 4 SYM theory, the d = 3 N = 2 SCSM theory, and the ABJM theory

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Summary

Straight lines and circles in Minkowski spacetime

We consider the BPS Wilson loops along infinite straight lines and circles in several supersymmetric conformal field theories in Minkowski spacetime. There is no spacelike 1/2 BPS Wilson loop along an infinite straight line in N = 4 SYM theory in d = 4 Minkowski spacetime. Since the d = 4 N = 4 SYM theory is a superconformal theory and an infinite straight line can be mapped to a circle by an appropriate conformal transformation, there is no spacelike 1/2 BPS Wilson loop along a circle either.. One gets a 1/2 BPS Wilson loop along a timelike infinite straight line. We conclude that there is no 1/2 BPS Wilson loop along a spacelike infinite straight line in N = 2 SCSM theory. There is a conformal transformation that turns a spacelike infinite straight line into a circle, and so there is no 1/2 BPS Wilson loop along a spacelike circle either

ABJM theory
Straight lines and circles in Euclidean space
General curves in Minkowski spacetime
DT type Wilson loop
Conclusion and discussion
A Majorana spinors in various dimensions
B Consistent constraints for Majorana spinors

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