1989
DOI: 10.1016/0370-2693(89)90029-4
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On the algebraic characterization of witten's topological Yang-Mills theory

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Cited by 121 publications
(97 citation statements)
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“…We adopt here the standard construction of refs. [17,18,19] and introduce the following set of fields: a gauge connection A a µ , an anticommuting vector field ψ a µ (also called topological ghost), a pair of antiself-dual tensor fields (B a µν , χ a µν ) and two ghost fields (c a , ϕ a ). One needs also a couple of Lagrange multipliers (b a , η a ) and a couple of antighosts (c a ,φ a ).…”
Section: The Classical Action and The Landau Gaugementioning
confidence: 99%
“…We adopt here the standard construction of refs. [17,18,19] and introduce the following set of fields: a gauge connection A a µ , an anticommuting vector field ψ a µ (also called topological ghost), a pair of antiself-dual tensor fields (B a µν , χ a µν ) and two ghost fields (c a , ϕ a ). One needs also a couple of Lagrange multipliers (b a , η a ) and a couple of antighosts (c a ,φ a ).…”
Section: The Classical Action and The Landau Gaugementioning
confidence: 99%
“…Generators generated by the first two functions coincide with the corresponding generators of the standard BRST model (arising in the 4d topological Yang-Mills theory [7]) to which the Kalkman model is reduced at t = 1. The function D 1 generates the differential different from the standard BRST onê…”
Section: Models For Equivariant Cohomologymentioning
confidence: 97%
“…The algebra Ω(M ) ⊗ W(g) and the differential (21) form the BRST model of equivariant cohomology [12,30]. However, this complex is a model for M × EG (hence its cohomology is equal to H…”
Section: The Algebroid Structure Of [−1]t a Is As Follows The Anchormentioning
confidence: 99%