English

On $3$-gauge transformations, $3$-curvature and $\mathbf{Gray}$-categories

Mathematical Physics 2015-06-17 v2 High Energy Physics - Theory Category Theory Differential Geometry math.MP

Abstract

In the 33-gauge theory, a 33-connection is given by a 11-form AA valued in the Lie algebra g \mathfrak g, a 22-form BB valued in the Lie algebra h\mathfrak h and a 33-form CC valued in the Lie algebra l \mathfrak l , where (g,h,l)(\mathfrak g,\mathfrak h, \mathfrak l) constitutes a differential 2 2-crossed module. We give the 33-gauge transformations from a 33-connection to another, and show the transformation formulae of the 11-curvature 22-form, the 22-curvature 33-form and the 33-curvature 44-form. The gauge configurations can be interpreted as smooth Gray\mathbf{Gray}-functors between two Gray\mathbf{Gray} 33-groupoids: the path 33-groupoid P3(X)\mathcal{P}_3(X) and the 33-gauge group GL \mathcal{G}^{\mathscr L} associated to the 2 2-crossed module L\mathscr L, whose differential is (g,h,l)(\mathfrak g,\mathfrak h, \mathfrak l). The derivatives of Gray\mathbf{Gray}-functors are 33-connections, and the derivatives of lax-natural transformations between two such Gray\mathbf{Gray}-functors are 33-gauge transformations. We give the 33-dimensional holonomy, the lattice version of the 33-curvature, whose derivative gives the 33-curvature 44-form. The covariance of 33-curvatures easily follows from this construction. This Gray\mathbf{ Gray}-categorical construction explains why 33-gauge transformations and 33-curvatures have the given forms. The interchanging 33-arrows are responsible for the appearance of terms concerning the Peiffer commutator {,}\{,\}.

Cite

@article{arxiv.1311.3796,
  title  = {On $3$-gauge transformations, $3$-curvature and $\mathbf{Gray}$-categories},
  author = {Wei Wang},
  journal= {arXiv preprint arXiv:1311.3796},
  year   = {2015}
}

Comments

36 pages

R2 v1 2026-06-22T02:08:10.741Z