Results 121 to 130 of about 7,720 (196)

Miura operators, degenerate fields and the M2-M5 intersection. [PDF]

J High Energy Phys, 2022
Gaiotto D, Rapčák M.
europepmc   +1 more source

Auxialiary conditions in BRST quantization

Nuclear Physics B, 1992
Abstract A general structure of allowed auxiliary conditions in both ordinary and generalized BRST quantization is presented. Such conditions are shown to fall into two classes which always should imply each other. Both antiBRST invariance and coBRST invariance are shown to fit into the framework.
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Combinatorial proof of a non-renormalization theorem

Journal of High Energy Physics
We provide a direct combinatorial proof of a Feynman graph identity which implies a wide generalization of a formality theorem by Kontsevich. For a Feynman graph Γ, we associate to each vertex a position x v ∈ ℝ and to each edge e the combination s e = a
Paul-Hermann Balduf, Davide Gaiotto
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Hamiltonian BRST quantization of the conformal spinning string [PDF]

, 1995
P. Saltsidis
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A ∞ action of open $$\mathcal{N}=2$$ superstring field theory

Journal of High Energy Physics
We formulate a string field theory for open $$\mathcal{N}=2$$ strings with an A ∞ algebra structure. Starting from the BRST cohomology relative to the U(1) anti-ghost zero-mode, we generalize [arXiv:1312.2948] and constructed all interacting vertices ...
Xianghang Zhang
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Entanglement entropy and edge modes in topological string theory. Part I. Generalized entropy for closed strings. [PDF]

J High Energy Phys, 2021
Donnelly W, Jiang Y, Kim M, Wong G.
europepmc   +1 more source

Off-shell Gauge Fields from BRST Quantization [PDF]

, 2006
Maxim Grigoriev
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BRST quantization of spinning relativistic particles with extended supersymmetries

, 1990
Michelle Pierri, Victor O. Rivelles
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Geometry and Topology of Anti-BRST Symmetry in Quantized Yang-Mills\n Gauge Theories [PDF]

, 2020
Amir Abbass Varshovi
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BRST quantization of the superparticle

Physics Letters B, 1988
Abstract We show that the quantization of the superparticle action is possible. This is done by shifts in the BRST operator and the resulting action has an infinite number of ghosts. The total BRST operator is given by an infinite sum and is shown to be nilpotent. We also obtain a BRST invariant kinetic operator that contains the dynamical, auxiliary
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