Search results for "Symplectic geometry"

showing 10 items of 209 documents

古典波動現象のトポロジーによる特徴付け; 静磁スピン波表面モードのトポロジカルな起源

2019

We propose a topological characterization of Hamiltonians describing classical waves. Applying it to the magnetostatic surface spin waves that are important in spintronics applications, we settle the speculation over their topological origin. For a class of classical systems that includes spin waves driven by dipole-dipole interactions, we show that the topology is characterized by vortex lines in the Brillouin zone in such a way that the symplectic structure of Hamiltonian mechanics plays an essential role. We define winding numbers around these vortex lines and identify them to be the bulk topological invariants for a class of semimetals. Exploiting the bulk-edge correspondence appropriat…

Hamiltonian mechanicsSurface (mathematics)PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsSpintronicsFOS: Physical sciencesGeneral Physics and AstronomyPhysik (inkl. Astronomie)Topology01 natural sciencesVortexBrillouin zonesymbols.namesakeSpin waveMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencessymbols010306 general physicsTopology (chemistry)Symplectic geometryPhysical review letters
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Geodesics on spaces of almost hermitian structures

1994

A natural metric on the space of all almost hermitian structures on a given manifold is investigated.

Hermitian symmetric spacePure mathematicsGeodesicGeneral MathematicsMathematical analysisSpace (mathematics)Fubini–Study metricHermitian matrixMetric (mathematics)Hermitian manifoldMathematics::Differential GeometryComplex manifoldMathematics::Symplectic GeometryMathematicsIsrael Journal of Mathematics
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The Complete Solution of the Classical SL(2,ℝ/U(1) Gauged WZNW Field Theory

1998

We prove that any gauged WZNW model has a Lax pair representation, and give explicitly the general solution of the classical equations of motion of the SL(2,R)/U(1) theory. We calculate the symplectic structure of this solution by solving a differential equation of the Gelfand-Dikii type with initial state conditions at infinity, and transform the canonical physical fields non-locally onto canonical free fields. The results will, finally, be collected in a local B\"acklund transformation. These calculations prepare the theory for an exact canonical quantization.

High Energy Physics - TheoryDifferential equationCanonical quantizationFOS: Physical sciencesEquations of motionStatistical and Nonlinear PhysicsState (functional analysis)Type (model theory)Nonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Lax pairField theory (psychology)Mathematical PhysicsSymplectic geometryMathematical physicsMathematicsCommunications in Mathematical Physics
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Real symplectic formulation of local special geometry

2006

We consider a formulation of local special geometry in terms of Darboux special coordinates $P^I=(p^i,q_i)$, $I=1,...,2n$. A general formula for the metric is obtained which is manifestly $\mathbf{Sp}(2n,\mathbb{R})$ covariant. Unlike the rigid case the metric is not given by the Hessian of the real function $S(P)$ which is the Legendre transform of the imaginary part of the holomorphic prepotential. Rather it is given by an expression that contains $S$, its Hessian and the conjugate momenta $S_I=\frac{\partial S}{\partial P^I}$. Only in the one-dimensional case ($n=1$) is the real (two-dimensional) metric proportional to the Hessian with an appropriate conformal factor.

High Energy Physics - TheoryHessian matrixPhysicsPure mathematicsNuclear and High Energy PhysicsHolomorphic functionFOS: Physical sciencesLegendre functionLegendre transformationsymbols.namesakeAssociated Legendre polynomialsHigh Energy Physics - Theory (hep-th)Real-valued functionMetric (mathematics)symbolsParticle Physics - TheorySymplectic geometryPhysics Letters B
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The Schouten - Nijenhuis bracket, cohomology and generalized Poisson structures

1996

Newly introduced generalized Poisson structures based on suitable skew-symmetric contravariant tensors of even order are discussed in terms of the Schouten-Nijenhuis bracket. The associated `Jacobi identities' are expressed as conditions on these tensors, the cohomological contents of which is given. In particular, we determine the linear generalized Poisson structures which can be constructed on the dual spaces of simple Lie algebras.

High Energy Physics - TheoryMathematics - Differential GeometryPhysicsPure mathematicsSchouten–Nijenhuis bracketFOS: Physical sciencesGeneral Physics and AstronomyOrder (ring theory)Statistical and Nonlinear PhysicsPoisson distributionCohomologysymbols.namesakeBracket (mathematics)High Energy Physics - Theory (hep-th)Differential Geometry (math.DG)Simple (abstract algebra)Mathematics - Quantum AlgebraLie algebraFOS: MathematicssymbolsCovariance and contravariance of vectorsQuantum Algebra (math.QA)Mathematics::Symplectic GeometryMathematical PhysicsJournal of Physics A: Mathematical and General
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Conifold Transitions and Mirror Symmetry for Calabi-Yau Complete Intersections in Grassmannians

1997

In this paper we show that conifold transitions between Calabi-Yau 3-folds can be used for the construction of mirror manifolds and for the computation of the instanton numbers of rational curves on complete intersection Calabi-Yau 3-folds in Grassmannians. Using a natural degeneration of Grassmannians $G(k,n)$ to some Gorenstein toric Fano varieties $P(k,n)$ with conifolds singularities which was recently described by Sturmfels, we suggest an explicit mirror construction for Calabi-Yau complete intersections $X \subset G(k,n)$ of arbitrary dimension. Our mirror construction is consistent with the formula for the Lax operator conjectured by Eguchi, Hori and Xiong for gravitational quantum c…

High Energy Physics - TheoryNuclear and High Energy PhysicsInstantonPure mathematicsConifoldComplete intersectionFOS: Physical sciencesFano planeMathematics - Algebraic GeometryMathematics::Algebraic GeometryHigh Energy Physics - Theory (hep-th)FOS: MathematicsCalabi–Yau manifoldGravitational singularityMathematics::Differential GeometryMirror symmetryAlgebraic Geometry (math.AG)Mathematics::Symplectic GeometryQuantum cohomologyMathematics
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Tracing symmetries and their breakdown through phases of heterotic (2,2) compactifications

2015

We are considering the class of heterotic $\mathcal{N}=(2,2)$ Landau-Ginzburg orbifolds with 9 fields corresponding to $A_1^9$ Gepner models. We classify all of its Abelian discrete quotients and obtain 152 inequivalent models closed under mirror symmetry with $\mathcal{N}=1,2$ and $4$ supersymmetry in 4D. We compute the full massless matter spectrum at the Fermat locus and find a universal relation satisfied by all models. In addition we give prescriptions of how to compute all quantum numbers of the 4D states including their discrete R-symmetries. Using mirror symmetry of rigid geometries we describe orbifold and smooth Calabi-Yau phases as deformations away from the Landau-Ginzburg Ferma…

High Energy Physics - TheoryPhysicsHeterotic string theoryNuclear and High Energy Physics010308 nuclear & particles physicsFOS: Physical sciencesTorusSupersymmetry01 natural sciencesHigh Energy Physics::Theorysymbols.namesakeHigh Energy Physics - Theory (hep-th)0103 physical sciencesHomogeneous spacesymbolsAbelian group010306 general physicsMirror symmetryMathematics::Symplectic GeometryHiggs mechanismOrbifoldMathematical physicsJournal of High Energy Physics
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Non-extremal black holes of N = 2, d = 4 supergravity

2011

We propose a generic recipe for deforming extremal black holes into non-extremal black holes and we use it to find and study the non-extremal black-hole solutions of several N=2,d=4 supergravity models (SL(2,R)/U(1), CPn and STU with four charges). In all the cases considered, the non-extremal family of solutions smoothly interpolates between all the different extremal limits, supersymmetric and not supersymmetric. This fact can be used to find explicitly extremal non-supersymmetric solutions in the cases in which the attractor mechanism does not completely fix the values of the scalars on the event horizon and they still depend on the boundary conditions at spatial infinity. We compare (su…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsEvent horizonSupergravitySuperpotentialFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyModuli spaceBlack holeCombinatoricsHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)AttractorCentral chargeSymplectic geometryJournal of High Energy Physics
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Observations on the Darboux coordinates for rigid special geometry

2006

We exploit some relations which exist when (rigid) special geometry is formulated in real symplectic special coordinates $P^I=(p^\Lambda,q_\Lambda), I=1,...,2n$. The central role of the real $2n\times 2n$ matrix $M(\Re \mathcal{F},\Im \mathcal{F})$, where $\mathcal{F} = \partial_\Lambda\partial_\Sigma F$ and $F$ is the holomorphic prepotential, is elucidated in the real formalism. The property $M\Omega M=\Omega$ with $\Omega$ being the invariant symplectic form is used to prove several identities in the Darboux formulation. In this setting the matrix $M$ coincides with the (negative of the) Hessian matrix $H(S)=\frac{\partial^2 S}{\partial P^I\partial P^J}$ of a certain hamiltonian real fun…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsPure mathematicsHolomorphic functionFOS: Physical sciencesKähler manifoldsymbols.namesakeHigh Energy Physics - Theory (hep-th)Real-valued functionsymbolsMathematics::Differential GeometryComplex manifoldInvariant (mathematics)Hamiltonian (quantum mechanics)Mathematics::Symplectic GeometryParticle Physics - TheoryHyperkähler manifoldSymplectic geometryJournal of High Energy Physics
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N=2 Super-Higgs, N=1 Poincare' Vacua and Quaternionic Geometry

2002

In the context of N=2 supergravity we explain the occurrence of partial super-Higgs with vanishing vacuum energy and moduli stabilization in a model suggested by superstring compactifications on type IIB orientifolds with 3-form fluxes. The gauging of axion symmetries of the quaternionic manifold, together with the use of degenerate symplectic sections for special geometry, are the essential ingredients of the construction.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSupergravityHigh Energy Physics::PhenomenologySuperstring theoryFOS: Physical sciencesContext (language use)Partícules (Física nuclear)ModuliHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Homogeneous spaceHiggs bosonAxionMathematics::Symplectic GeometryParticle Physics - TheorySymplectic geometryMathematical physics
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