1997
DOI: 10.4064/-39-1-211-223
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Quantum Fibre Bundles. An Introduction

Abstract: Abstract. An approach to construction of a quantum group gauge theory based on the quantum group generalisation of fibre bundles is reviewed.

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“…The monopole connection corresponds to the choice U = V = 0 ⇔ a = 0, so to have Π 0 (ω z ) = ω z and the monopole connection 1-form ω 0 (z j ) = [(1 − q −2j )/(1 − q −2 )]ω z [5,9]. With a connection, one has the notion of covariant derivative D : A(SU q (2)) → Ω 1 (A(SU q (2))) of equivariant maps.…”
Section: Vertical Subspaces On the Quantum Hopf Bundle The Right Coamentioning
confidence: 99%
“…The monopole connection corresponds to the choice U = V = 0 ⇔ a = 0, so to have Π 0 (ω z ) = ω z and the monopole connection 1-form ω 0 (z j ) = [(1 − q −2j )/(1 − q −2 )]ω z [5,9]. With a connection, one has the notion of covariant derivative D : A(SU q (2)) → Ω 1 (A(SU q (2))) of equivariant maps.…”
Section: Vertical Subspaces On the Quantum Hopf Bundle The Right Coamentioning
confidence: 99%