2015
DOI: 10.1140/epjc/s10052-015-3529-z
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Yang–Mills theory for semidirect products $$\mathrm{G}\ltimes \mathfrak {g}^*$$ G ⋉ g ∗ and its instantons

Abstract: Dedicated to Ramón F. Alvarez-Estrada on occasion of his 70th birthday Yang-Mills theory with a symmetry algebra that is the semidirect product h ⋉ h * defined by the coadjoint action of a Lie algebra h on its dual h * is studied. The gauge group is the semidirect product G h ⋉ h * , a noncompact group given by the coadjoint action on h * of the Lie group G h of h. For h simple, a method to construct the self-antiself dual instantons of the theory and their gauge nonequivalent deformations is presented. Every … Show more

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Cited by 1 publication
(3 citation statements)
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“…The pattern observed for the gauge invariant degrees of freedom in the quantum theory resembles very much that for the self-antiself dual instantons of the classical theory [16]. In the classical case, the number of collective coordinates of the G ⋉ instantons is twice that of the embedded G instantons, yet ω ab F a Tµν F bµν Z does not contribute to the instanton number.…”
Section: Discussionmentioning
confidence: 62%
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“…The pattern observed for the gauge invariant degrees of freedom in the quantum theory resembles very much that for the self-antiself dual instantons of the classical theory [16]. In the classical case, the number of collective coordinates of the G ⋉ instantons is twice that of the embedded G instantons, yet ω ab F a Tµν F bµν Z does not contribute to the instanton number.…”
Section: Discussionmentioning
confidence: 62%
“…So far no restriction has been placed on g. Assume now that it is semisimple. In this case, g ⋉ can be viewed as a limit of the direct product of g with itself [16]. To see this, take ω ab in eq.…”
Section: Semidirect Products Of Lie Algebras and Their Groupsmentioning
confidence: 99%
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