Results 81 to 90 of about 291 (152)
On Globalized Traces for the Poisson Sigma Model. [PDF]
Commun Math Phys, 2022 Moshayedi N.
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Worldline formulations of covariant fracton theories
European Physical Journal C: Particles and FieldsWe develop worldline formulations of covariant fracton gauge theories. These are a one-parameter family of gauge theories of a rank-two symmetric tensor field, invariant under a scalar gauge transformation involving a double derivative.
Filippo Fecit, Davide Rovere
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On BRST-related symmetries in the FLPR model with Gribov ambiguities
Nuclear Physics BWith the recent revival of interest in the FLPR model, novel features have been reported in the literature. A connection between those new feautures and QCD, involving the Gribov problem, is explored.
Bhabani Prasad Mandal +2 more
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Geometric quantization of the BRST charge [PDF]
Communications in Mathematical Physics, 1992 zbMATH Open Web Interface contents unavailable due to conflicting licenses.
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Families of gauge conditions in BV formalism
Journal of High Energy Physics, 2017 In BV formalism we can consider a Lagrangian submanifold as a gauge condition. Starting with the BV action functional we construct a closed form on the space of Lagrangian submanifolds.
Andrei Mikhailov, Albert Schwarz
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Quantum Chern-Simons Theories on Cylinders: BV-BFV Partition Functions. [PDF]
Commun Math Phys, 2023 Cattaneo AS, Mnev P, Wernli K.
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The algebraic structure of BRST quantization
Physics Letters B, 1986 Abstract It is shown that a system of first-class bosonic constraints obeying a Lie algebra has associated with it a natural superalgebra. BRST quantization arises as a non-linear representation of this superalgebra. Two distinct superalgebras are explicitly constructed and their associated BRST quantizations presented. The first BRST quantization is
Mark J. Bowick, Feza Gürsey
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Simplified D = 11 pure spinor b ghost
Journal of High Energy Physics, 2017 A b-ghost was constructed for the D = 11 non-minimal pure spinor superparticle by requiring that {Q, b} = T where Q = Λ α D α + R α W ¯ α $$ Q={\Lambda}^{\alpha }{D}_{\alpha }+{R}^{\alpha }{\overline{W}}_{\alpha } $$ is the usual non-minimal pure spinor ...
Nathan Berkovits, Max Guillen
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On the M2-Brane Index on Noncommutative Crepant Resolutions. [PDF]
Lett Math Phys, 2022 Cirafici M.
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Asymptotic Symmetries in the BV-BFV Formalism. [PDF]
Commun Math Phys, 2021 Rejzner K, Schiavina M.
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