Quantum Principal Bundles
Table of Contents
Introduction
Differential Calculus
Connections Formalism
Characteristic Classes
Quantum Classifying Spaces
Quantum Frame Bundles
Associated Bundles
Gauge Transformations
Literature
Quantum Frame Bundles
A very interesting class of quantum principal
bundles is given by frame bundles. They provide a nice working framework to
incorporate various geometrical structures (including Riemannian, symplectic,
complex and spin structures) into the quantum context. The main idea is to define
quantum frame bundles axiomatically, as in the classical geometry [KN], starting from the
idea of cannonical coordinate first-order horizontal forms. In classical geometry,
the algebra of horizontal forms is realizable as the tensor product of the functions
on the bundle with the exterior algebra associated to the space of coordinate first-order
forms. This property can be used [D10] as a starting point in defining quantum frame bundles-in
quantum case the space of horizontal forms is defined as
where
is a vector space defining quantum first-order horizontal forms, and
is a braided exterior algebra built over
,
relative to the appropriate braid operator
.
This braid operator comes from the theory of bicovariant bimodules
[W3]--because it is assumed that
is a left-invariant part of a bicovariant *-bimodule
over G. This also implies that G is naturally acting by a *-homomorphism
Taking a product of the actions F and
we can define the structure quantum group action
It is important to mention that the algebra structure on
hor(P) is not a simple tensor product, but the appropriate cross-product
of
and
so that above mentioned structure group coaction is a *-homomorphism. To complete
the geometrical picture of a quantum frame bundle, it is necessary to postulate
the existence of the appropriate differential calculus on the *-algebra
of
G-invariant elements of hor(P).
Quantum frame bundles also provide a class of examples of principal bundles
where it is possible to built an intrinsic differential caclulus
on the bundle,
applying a general constructive approach to differential calculi, developed in [D6]. In the
framework of such a calculus, it is possible to incorporate into the quantum context
the entire formalism of torsion operators, and to generalize various important
constructions of clasical Riemannian/spin geometry--including the study of Levi-Civita
connections and constructions of a quantum Dirac operator [D10][D11].
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