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- 't_Hooft_operator abstract "In theoretical physics, a 't Hooft operator, introduced by Gerard 't Hooft in the 1978 paper "On the phase transition towards permanent quark confinement", is a dual version of the Wilson loop in which the electromagnetic potential A is replaced by its electromagnetic dual Amag, where the exterior derivative of A is equal to the Hodge dual of the exterior derivative of Amag. In d spacetime dimensions, Amag is a (d-3)-form and so the 't Hooft operator is the integral of Amag over a (d-3)-dimensional surface.".
- 't_Hooft_operator wikiPageExternalLink 0212264v1.
- 't_Hooft_operator wikiPageExternalLink 14157.pdf.
- 't_Hooft_operator wikiPageID "3386119".
- 't_Hooft_operator wikiPageRevisionID "527501499".
- 't_Hooft_operator hasPhotoCollection 't_Hooft_operator.
- 't_Hooft_operator subject Category:Quantum_field_theory.
- 't_Hooft_operator comment "In theoretical physics, a 't Hooft operator, introduced by Gerard 't Hooft in the 1978 paper "On the phase transition towards permanent quark confinement", is a dual version of the Wilson loop in which the electromagnetic potential A is replaced by its electromagnetic dual Amag, where the exterior derivative of A is equal to the Hodge dual of the exterior derivative of Amag.".
- 't_Hooft_operator label "'t Hooft operator".
- 't_Hooft_operator sameAs m.098wxv.
- 't_Hooft_operator sameAs Q4540599.
- 't_Hooft_operator sameAs Q4540599.
- 't_Hooft_operator wasDerivedFrom 't_Hooft_operator?oldid=527501499.
- 't_Hooft_operator isPrimaryTopicOf 't_Hooft_operator.