My recent
article: G.Sardanashvily, “Classical Higgs fields” in arXiv: 1602.03818
We consider
classical gauge theory on a principal bundle P->X in a case of spontaneous symmetry breaking characterized by
the reduction of a structure group G
of P->X to its closed subgroup H. This reduction is ensured by the
existence of global sections of the quotient bundle P/H->X treated as classical Higgs fields. Matter fields with an
exact symmetry group H in such gauge
theory are considered in the pairs with Higgs fields, and they are represented
by sections of a composite bundle Y->P/H->X,
where Y->P/H is a fiber bundle
associated to a principal bundle P->P/H
with a structure group H. A key point
is that a composite bundle Y->X is
proved to be associated to a principal G-bundle
P->X. Therefore, though matter
fields possess an exact symmetry group H,
their gauge G-invariant theory in the
presence of Higgs fields can be developed. Its gauge invariant Lagrangian
factorizes through the vertical covariant differential determined by a
connection on a principal H-bundle P->P/H. In a case of the Cartan
decomposition of a Lie algebra of G,
this connection can be expressed in terms of a connection on a principal bundle
P->X, i.e., gauge potentials for a
group of broken symmetries G.
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