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16,559
ElectricMagnetic duality and the geometric . . .
, 2006
"... The geometric Langlands program can be described in a natural way by compactifying on a Riemann surface C a twisted version of N = 4 super YangMills theory in four dimensions. The key ingredients are electricmagnetic duality of gauge theory, mirror symmetry of sigmamodels, branes, Wilson and ’t H ..."
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Cited by 3 (0 self)
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The geometric Langlands program can be described in a natural way by compactifying on a Riemann surface C a twisted version of N = 4 super YangMills theory in four dimensions. The key ingredients are electricmagnetic duality of gauge theory, mirror symmetry of sigmamodels, branes, Wilson and ’t
Electricmagnetic dualities in supergravity, Nucl. Phys
 B (Proc. Suppl.), 101 (2001) 154, proc. Thirty Years of Supersymmetry
"... I review electricmagnetic duality from the perspective of extended supergravity theories in four spacetime dimensions. ..."
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Cited by 17 (7 self)
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I review electricmagnetic duality from the perspective of extended supergravity theories in four spacetime dimensions.
ElectricMagnetic duality and the geometric Langlands program
, 2006
"... The geometric Langlands program can be described in a natural way by compactifying on a Riemann surface C a twisted version of N = 4 super YangMills theory in four dimensions. The key ingredients are electricmagnetic duality of gauge theory, mirror symmetry of sigmamodels, branes, Wilson and ’t H ..."
Abstract

Cited by 300 (26 self)
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The geometric Langlands program can be described in a natural way by compactifying on a Riemann surface C a twisted version of N = 4 super YangMills theory in four dimensions. The key ingredients are electricmagnetic duality of gauge theory, mirror symmetry of sigmamodels, branes, Wilson and ’t
Electricmagnetic duality rotations in nonlinear electrodynamics
 Nucl. Phys. B
, 1995
"... We show that there is a function of one variable’s worth of Lagrangians for a single Maxwell field coupled to gravity whose equations of motion admit electricmagnetic duality. Such Lagrangians are given by solutions of the HamiltonJacobi equation for timelike geodesics in Witten’s twodimensional ..."
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Cited by 34 (0 self)
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We show that there is a function of one variable’s worth of Lagrangians for a single Maxwell field coupled to gravity whose equations of motion admit electricmagnetic duality. Such Lagrangians are given by solutions of the HamiltonJacobi equation for timelike geodesics in Witten’s two
Can (electricmagnetic) duality be gauged
 Phys.Rev. D83 (2011) 045031, [arXiv:1011.5889
"... ar ..."
ElectricMagnetic Duality Invariant Lagrangians
, 1999
"... We find general nonlinear lagrangians of a U(1) field invariant under electricmagnetic duality. They are characterized by an arbitrary function and go to the Maxwell theory in the weak field limit. We give some explicit examples which are generalizations of the BornInfeld theory. ..."
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Cited by 5 (0 self)
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We find general nonlinear lagrangians of a U(1) field invariant under electricmagnetic duality. They are characterized by an arbitrary function and go to the Maxwell theory in the weak field limit. We give some explicit examples which are generalizations of the BornInfeld theory.
ElectricMagnetic Duality in Massless QED?
, 909
"... The possibility that QED and recently developed nonHermitian, or magnetic, versions of QED are equivalent is considered. Under this duality the Hamiltonians and anomalous axial currents of the two theories are identified. A consequence of such a duality is that particles described by QED carry magn ..."
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The possibility that QED and recently developed nonHermitian, or magnetic, versions of QED are equivalent is considered. Under this duality the Hamiltonians and anomalous axial currents of the two theories are identified. A consequence of such a duality is that particles described by QED carry
Electricmagnetic Duality in Noncommutative Geometry
, 1997
"... The structure of Sduality in U(1) gauge theory on a 4manifold M is examined using the formalism of noncommutative geometry. A noncommutative space is constructed from the algebra of Wilson’t Hooft line operators which encodes both the ordinary geometry of M and its infinitedimensional loop space ..."
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The structure of Sduality in U(1) gauge theory on a 4manifold M is examined using the formalism of noncommutative geometry. A noncommutative space is constructed from the algebra of Wilson’t Hooft line operators which encodes both the ordinary geometry of M and its infinitedimensional loop
Results 1  10
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16,559