Leibniz-Yang-Mills Gauge Theories and the 2-Higgs Mechanism
arXiv:1903.07365 · doi:10.1103/PhysRevD.99.115026
Abstract
A quadratic Leibniz algebra gives rise to a canonical Yang-Mills type functional over every space-time manifold. The gauge fields consist of 1-forms taking values in and 2-forms with values in the subspace generated by the symmetric part of the bracket. If the Leibniz bracket is anti-symmetric, the quadratic Leibniz algebra reduces to a quadratic Lie algebra, , and becomes identical to the usual Yang-Mills action functional. We describe this gauge theory for a general quadratic Leibniz algebra. We then prove its (classical and quantum) equivalence to a Yang-Mills theory for the Lie algebra to which one couples massive 2-form fields living in a -representation. Since in the original formulation the B-fields have their own gauge symmetry, this equivalence can be used as an elegant mass-generating mechanism for 2-form gauge fields, thus providing a 'higher Higgs mechanism' for those fields.
6 pages; a subsection with remarks on finite gauge transformations added. Version to be published in Phys. Rev. D
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