Does the nontrivially deformed field-antifield formalism exist?
Abstract
We reformulate the Lagrange deformed field-antifield BV -formalism suggested, in terms of the general Euler vector field N generated by the antisymplectic potential. That N generalizes, in a natural anticanonically-invariant manner, the usual power-counting operator. We provide for the "usual" gauge-fixing mechanism as applied to the deformed BV -formalism.
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