Gauge gravitation theory should not be confused with the similarly named gauge theory gravity, which is a formulation of (classical) gravitation in the language of geometric algebra.
The first gauge model of gravity was suggested by Ryoyu Utiyama (1916–1990) in 1956[1] just two years after birth of the gauge theory itself.
[2] However, the initial attempts to construct the gauge theory of gravity by analogy with the gauge models of internal symmetries encountered a problem of treating general covariant transformations and establishing the gauge status of a pseudo-Riemannian metric (a tetrad field).
In order to overcome this drawback, representing tetrad fields as gauge fields of the translation group was attempted.
[3] Infinitesimal generators of general covariant transformations were considered as those of the translation gauge group, and a tetrad (coframe) field was identified with the translation part of an affine connection on a world manifold
There are different physical interpretations of the translation part
In gauge theory of dislocations, a field
motivates many authors to treat a coframe
[5] Difficulties of constructing gauge gravitation theory by analogy with the Yang–Mills one result from the gauge transformations in these theories belonging to different classes.
In the case of internal symmetries, the gauge transformations are just vertical automorphisms of a principal bundle
On the other hand, gravitation theory is built on the principal bundle
General covariant transformations are sufficient in order to restate Einstein's general relativity and metric-affine gravitation theory as the gauge ones.
In terms of gauge theory on natural bundles, gauge fields are linear connections on a world manifold
, defined as principal connections on the linear frame bundle
, and a metric (tetrad) gravitational field plays the role of a Higgs field responsible for spontaneous symmetry breaking of general covariant transformations.
[7] Spontaneous symmetry breaking is a quantum effect when the vacuum is not invariant under the transformation group.
In classical gauge theory, spontaneous symmetry breaking occurs if the structure group
[8] By virtue of the well-known theorem, there exists one-to-one correspondence between the reduced principal subbundles of
These sections are treated as classical Higgs fields.
The idea of the pseudo-Riemannian metric as a Higgs field appeared while constructing non-linear (induced) representations of the general linear group GL(4, R), of which the Lorentz group is a Cartan subgroup.
[9] The geometric equivalence principle postulating the existence of a reference frame in which Lorentz invariants are defined on the whole world manifold is the theoretical justification for the reduction of the structure group GL(4, R) of the linear frame bundle FX to the Lorentz group.
Then the very definition of a pseudo-Riemannian metric on a manifold
as a global section of the quotient bundle FX / O(1, 3) → X leads to its physical interpretation as a Higgs field.
The physical reason for world symmetry breaking is the existence of Dirac fermion matter, whose symmetry group is the universal two-sheeted covering SL(2, C) of the restricted Lorentz group, SO+(1, 3).