1996
DOI: 10.1016/0370-2693(96)00879-9
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Note on constrained cohomology

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1996
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Cited by 18 publications
(29 citation statements)
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“…We observe that this is true only because we are assuming that the original global symmetries are Abelian (eqs. (13)). Now, the process of gauging the symmetry associated to the set of parameters ǫ a does not modify the form of the generators R m α and R r α .…”
Section: Global Abelian Anomalies In the Bv Quantizationmentioning
confidence: 99%
“…We observe that this is true only because we are assuming that the original global symmetries are Abelian (eqs. (13)). Now, the process of gauging the symmetry associated to the set of parameters ǫ a does not modify the form of the generators R m α and R r α .…”
Section: Global Abelian Anomalies In the Bv Quantizationmentioning
confidence: 99%
“…[7]), constant ghosts are introduced of ghost number 1 and of Grassmann parity opposite to that of the symmetry parameter [8]. The Ward identities then follow by solving an extended master equation [8][9][10], the explicit form of which will be given below. This approach, which works even if the gauge-fixing procedure does not preserve manifest invariance under the rigid symmetry, has proved useful in the investigation of the renormalization and anomaly problems in globally supersymmetric models [11,12].…”
mentioning
confidence: 99%
“…The crucial point is that the cohomology of Q T is only non-trivial if one restricts the space of polynomials to those which are analytical in the global ghosts t, ǫ µ and t µ [16]. In fact, the cohomological classes are generated by monomials P n (φ) of the undifferentiated fields φ…”
Section: N=2 D=4 Sym and Topological Yang-millsmentioning
confidence: 99%
“…The analysis of the proof in [16] is based on a filtration of the functional space (which contains the constant ghosts t, ǫ µ , τ µ ), and of the BRST operator with respect to the counting operator N = t∂ t . One has Q T = 2 n=0 Q n , where…”
Section: N=2 D=4 Sym and Topological Yang-millsmentioning
confidence: 99%