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Compactified D=11 supermembranes and symplectic noncommutative gauge theories
It is shown that a double compactified D=11 supermembrane with nontrivial wrapping may be formulated as a symplectic noncommutative gauge theory on the world volume. The symplectic noncommutativeExpand
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Local Well-Posedness for Membranes in the Light Cone Gauge
In this paper we consider the classical initial value problem for the bosonic membrane in light cone gauge. A Hamiltonian reduction gives a system with one constraint, the area preserving constraint.Expand
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ON THE CONSISTENCY OF THE HOŘAVA THEORY
With the goal of giving evidence for the theoretical consistency of the Hořava theory, we perform a Hamiltonian analysis on a classical model suitable for analyzing its effective dynamics at largeExpand
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A global quadratic algorithm for solving a system of mixed equalities and inequalities
TLDR
A new algorithm is proposed which, under mild assumptions, generates a sequence{xi} that starting at any point inRn will converge to a setX defined by a mixed system of equations and inequalities. Expand
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New topological aspects of BF theories
BF theories defined over non-trivial line bundles are studied. It is shown that such theories describe a realization of a non-trivial higher-order bundle. The partition function differs from theExpand
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On the stability of compactified D = 11 supermembranes: Global aspects of the bosonic sector
We prove that the Hamiltonian for the bosonic sector of D = 11 supermembrane theories, wrapped in an irreducible way around S1 × S1 × M9 on the target manifold, only has strict minima withoutExpand
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Symplectic connections, Noncommutative Yang Mills theory and Supermembranes
Abstract In built noncommutativity of supermembranes with central charges in eleven dimensions is disclosed. This result is used to construct an action for a noncommutative supermembrane whereExpand
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Pure electromagnetic-gravitational interaction in Hořava–Lifshitz theory at the kinetic conformal point
We introduce the electromagnetic-gravitational coupling in the Hořava–Lifshitz framework, in $$3+1$$ 3 + 1 dimensions, by considering the Hořava–Lifshitz gravity theory in $$4+1$$ 4 + 1 dimensions atExpand
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Closure of the algebra of constraints for a nonprojectable Hořava model
We perform the Hamiltonian analysis for a nonprojectable Horava model whose potential is composed of R and R{sup 2} terms. We show that Dirac's algorithm for the preservation of the constraints canExpand
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Anisotropic coupling of gravity and electromagnetism in Hořava-Lifshitz theory
We analyze the electromagnetic-gravity interaction in a pure Hořava-Lifshitz framework. To do so we formulate the Hořava-Lifshitz gravity in $4+1$ dimensions and perform a Kaluza-Klein reduction toExpand
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