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Type IIB GreenSchwarz superstring in plane wave RamondRamond background
 Nucl. Phys. B
"... We construct the covariant κsymmetric superstring action for type IIB superstring on plane wave space supported by RamondRamond background. The action is defined as a 2d sigmamodel on the coset superspace. We fix the fermionic and bosonic lightcone gauges in the covariant GreenSchwarz superstri ..."
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Cited by 476 (0 self)
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We construct the covariant κsymmetric superstring action for type IIB superstring on plane wave space supported by RamondRamond background. The action is defined as a 2d sigmamodel on the coset superspace. We fix the fermionic and bosonic lightcone gauges in the covariant Green
The LightCone Gauge without Prescriptions
, 1999
"... Feynman integrals in the physical lightcone gauge are more difficult to solve than their covariant counterparts. The difficulty is associated with the presence of unphysical singularities due to the inherent residual gauge freedom in the intermediate boson propagators constrained within this gauge ..."
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stepwise consideration of causality, would be of great advantage. And this third option is realizable within the context of negative dimensions, or as it has been coined, the negative dimensional integration method (NDIM). The lightcone gauge in quantum field theory is a fascinating subject. It is a
Planar diagrams in lightcone gauge
 JHEP
, 2006
"... Preprint typeset in JHEP style PAPER VERSION ..."
The Schwinger Model in LightCone Gauge
, 1997
"... The Schwinger model, defined in the space interval −L ≤ x ≤ L, with (anti)periodic boundary conditions, is canonically quantized in the lightcone gauge A − = 0 by means of equaltime (anti)commutation relations. The transformation diagonalizing the complete Hamiltonian is explicitly constructed, th ..."
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The Schwinger model, defined in the space interval −L ≤ x ≤ L, with (anti)periodic boundary conditions, is canonically quantized in the lightcone gauge A − = 0 by means of equaltime (anti)commutation relations. The transformation diagonalizing the complete Hamiltonian is explicitly constructed
ChernSimons Gauge Theory as a String Theory
, 2003
"... Certain two dimensional topological field theories can be interpreted as string theory backgrounds in which the usual decoupling of ghosts and matter does not hold. Like ordinary string models, these can sometimes be given spacetime interpretations. For instance, threedimensional ChernSimons gaug ..."
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Cited by 551 (14 self)
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Simons gauge theory can arise as a string theory. The worldsheet model in this case involves a topological sigma model. Instanton contributions to the sigma model give rise to Wilson line insertions in the spacetime ChernSimons theory. A certain holomorphic analog of ChernSimons theory can also arise as a
The lightcone theorem
, 2009
"... We prove that the area of crosssections of lightcones, in spacetimes satisfying suitable energy conditions, is smaller than or equal to that of the corresponding crosssections in Minkowski, or de Sitter, or antide Sitter spacetime. The equality holds if and only if the metric coincides with th ..."
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Cited by 14 (4 self)
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We prove that the area of crosssections of lightcones, in spacetimes satisfying suitable energy conditions, is smaller than or equal to that of the corresponding crosssections in Minkowski, or de Sitter, or antide Sitter spacetime. The equality holds if and only if the metric coincides
LightCone Dynamics of Particles
, 1998
"... We review the foundations as well as a number of important applications of lightcone dynamics. Beginning with the peculiarities of relativistic particle dynamics we discuss the choice of a time parameter as the gauge fixing within reparametrization invariant dynamical systems. Including Poincaré in ..."
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We review the foundations as well as a number of important applications of lightcone dynamics. Beginning with the peculiarities of relativistic particle dynamics we discuss the choice of a time parameter as the gauge fixing within reparametrization invariant dynamical systems. Including Poincaré
Results 1  10
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536,819