Search results for "Integrable systems"

showing 10 items of 256 documents

Integrable systems and moduli spaces of curves

2016

This document has the purpose of presenting in an organic way my research on integrable systems originating from the geometry of moduli spaces of curves, with applications to Gromov-Witten theory and mirror symmetry. The text contains a short introduction to the main ideas and prerequisites of the subject from geometry and mathematical physics, followed by a synthetic review of some of my papers (listed below) starting from my PhD thesis (October 2008), and with some open questions and future developements. My results include: • the triple mirror symmetry among P 1-orbifolds with positive Euler characteristic , the Landau-Ginzburg model with superpotential −xyz + x p + y q + z r with 1 p + …

Espaces de modules de courbes[MATH.MATH-AG] Mathematics [math]/Algebraic Geometry [math.AG]mirror symmetrycohomological field theoriestautological ringsystèmes intégrablesintegrable systems[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]moduli spaces of stable curvesGromov-Witten theory[MATH.MATH-AG]Mathematics [math]/Algebraic Geometry [math.AG]quantization[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Mathematics::Symplectic Geometry
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Dissipative solitons for mode-locked lasers

2012

International audience; Dissipative solitons are localized formations of an electromagnetic field that are balanced through an energy exchange with the environment in presence of nonlinearity, dispersion and/or diffraction. Their growing use in the area of passively mode-locked lasers is remarkable: the concept of a dissipative soliton provides an excellent framework for understanding complex pulse dynamics and stimulates innovative cavity designs. Reciprocally, the field of mode-locked lasers serves as an ideal playground for testing the concept of dissipative solitons and revealing their unusual dynamics. This Review provides basic definitions of dissipative solitons, summarizes their imp…

Field (physics)NORMAL-DISPERSIONOPTICAL SOLITONSBOUND-STATES01 natural sciencesSIMILARITON FIBER LASERlaw.invention010309 opticsDissipative solitonOpticslawFiber laser0103 physical sciencesGINZBURG-LANDAU EQUATION010306 general physicsNonlinear Sciences::Pattern Formation and SolitonsCAVITY SOLITONSQuantum opticsPhysicsLOCALIZED STRUCTURESbusiness.industrySaturable absorptionLaserAtomic and Molecular Physics and OpticsSATURABLE-ABSORBERElectronic Optical and Magnetic MaterialsBiophotonicsNonlinear Sciences::Exactly Solvable and Integrable SystemsQuantum electrodynamicsDissipative systembusinessTI-SAPPHIRE LASERPULSE ENERGYNature Photonics
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Kondo Resonance in a Mesoscopic Ring Coupled to a Quantum Dot: Exact Results for the Aharonov-Bohm/Casher Effects

2000

We study the persistent currents induced by both the Aharonov-Bohm and Aharonov-Casher effects in a one-dimensional mesoscopic ring coupled to a side-branch quantum dot at Kondo resonance. For privileged values of the Aharonov-Bohm-Casher fluxes, the problem can be mapped onto an integrable model, exactly solvable by a Bethe ansatz. In the case of a pure magnetic Aharonov-Bohm flux, we find that the presence of the quantum dot has no effect on the persistent current. In contrast, the Kondo resonance interferes with the spin-dependent Aharonov-Casher effect to induce a current which, in the strong-coupling limit, is independent of the number of electrons in the ring.

General Physics and AstronomyFOS: Physical sciences02 engineering and technologyElectron01 natural sciencesResonance (particle physics)Bethe ansatzCondensed Matter - Strongly Correlated Electronssymbols.namesakeQuantum mechanics0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)010306 general physicsAharonov–Bohm effectPhysicsMesoscopic physicsCondensed Matter - Mesoscale and Nanoscale PhysicsNonlinear Sciences - Exactly Solvable and Integrable SystemsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Persistent currentQuantum Physics021001 nanoscience & nanotechnologyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectQuantum dotsymbolsKondo effectExactly Solvable and Integrable Systems (nlin.SI)0210 nano-technology
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On critical behaviour in systems of Hamiltonian partial differential equations

2013

Abstract We study the critical behaviour of solutions to weakly dispersive Hamiltonian systems considered as perturbations of elliptic and hyperbolic systems of hydrodynamic type with two components. We argue that near the critical point of gradient catastrophe of the dispersionless system, the solutions to a suitable initial value problem for the perturbed equations are approximately described by particular solutions to the Painlevé-I (P $$_I$$ I ) equation or its fourth-order analogue P $$_I^2$$ I 2 . As concrete examples, we discuss nonlinear Schrödinger equations in the semiclassical limit. A numerical study of these cases provides strong evidence in support of the conjecture.

Hamiltonian PDEsFOS: Physical sciencesSemiclassical physicsPainlevé equationsArticleSchrödinger equationHamiltonian systemsymbols.namesakeMathematics - Analysis of PDEs37K05Modelling and SimulationGradient catastrophe and elliptic umbilic catastrophe34M55FOS: MathematicsInitial value problemSettore MAT/07 - Fisica MatematicaEngineering(all)Mathematical PhysicsMathematicsG100Partial differential equationConjectureNonlinear Sciences - Exactly Solvable and Integrable SystemsHyperbolic and Elliptic systemsApplied MathematicsMathematical analysisQuasi-integrable systemsGeneral EngineeringMathematical Physics (math-ph)35Q55Nonlinear systemModeling and SimulationsymbolsExactly Solvable and Integrable Systems (nlin.SI)Hamiltonian (quantum mechanics)Gradient catastrophe and elliptic umbilic catastrophe; Hamiltonian PDEs; Hyperbolic and Elliptic systems; Painlevé equations; Quasi-integrable systemsAnalysis of PDEs (math.AP)
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Dimension bounds in monotonicity methods for the Helmholtz equation

2019

The article [B. Harrach, V. Pohjola, and M. Salo, Anal. PDE] established a monotonicity inequality for the Helmholtz equation and presented applications to shape detection and local uniqueness in inverse boundary problems. The monotonicity inequality states that if two scattering coefficients satisfy $q_1 \leq q_2$, then the corresponding Neumann-to-Dirichlet operators satisfy $\Lambda(q_1) \leq \Lambda(q_2)$ up to a finite-dimensional subspace. Here we improve the bounds for the dimension of this space. In particular, if $q_1$ and $q_2$ have the same number of positive Neumann eigenvalues, then the finite-dimensional space is trivial. peerReviewed

Helmholtz equationMathematics::Number Theorymontonicity methodMonotonic function01 natural sciencesinversio-ongelmatMathematics::Numerical AnalysisMathematics - Spectral TheoryMathematics - Analysis of PDEsDimension (vector space)FOS: MathematicsHelmholtz equationUniqueness0101 mathematicsSpectral Theory (math.SP)Mathematicsinverse problemsApplied Mathematics010102 general mathematicsMathematical analysisInverse problemMathematics::Spectral Theory010101 applied mathematicsComputational MathematicsNonlinear Sciences::Exactly Solvable and Integrable Systems35R30AnalysisAnalysis of PDEs (math.AP)
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Study of single top production at high energy electron positron colliders

2014

The effect of single top production on the study of top quark pair production in future high energy electron--positron colliders is evaluated. The rate of the single top quark production process is sizeable throughout a large range of center-of-mass energies and cannot easily be distinguished from the dominant pair production process. We discuss the impact on the top quark mass extraction from a scan through the pair production threshold and the determination of top quark form factors in the continuum. These results advocate for the exploration of the inclusive $e^+e^-\rightarrow W^+bW^-\bar{b}$ process, that includes both top quark pair and single top quark production.

High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics::PhenomenologyPhysics::Atomic and Molecular ClustersFOS: Physical sciencesHigh Energy Physics::ExperimentComputer Science::Computers and SocietyHigh Energy Physics - Experiment
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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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Abelian current algebra and the Virasoro algebra on the lattice

1993

We describe how a natural lattice analogue of the abelian current algebra combined with free discrete time dynamics gives rise to the lattice Virasoro algebra and corresponding hierarchy of conservation laws.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsConservation lawPure mathematicsHigh Energy Physics::Lattice010102 general mathematicsCurrent algebraFOS: Physical sciences01 natural sciencesNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Discrete time and continuous timeLattice (order)0103 physical sciencesVirasoro algebra0101 mathematicsAbelian group010306 general physicsPhysics Letters B
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Supersymmetry in non commutative superspaces

2003

Non commutative superspaces can be introduced as the Moyal-Weyl quantization of a Poisson bracket for classical superfields. Different deformations are studied corresponding to constant background fields in string theory. Supersymmetric and non supersymmetric deformations can be defined, depending on the differential operators used to define the Poisson bracket. Some examples of deformed, 4 dimensional lagrangians are given. For extended superspace (N>1), some new deformations can be defined, with no analogue in the N=1 case.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsFOS: Physical sciencesFísicaSupersymmetrySuperspaceString theoryDifferential operatorNoncommutative geometryPoisson bracketQuantization (physics)High Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Commutative propertyComputer Science::DatabasesParticle Physics - TheoryMathematical physics
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Lorentz harmonics and superfield action. D=10, N=1 superstring

2000

We propose a new version of the superfield action for a closed D=10, N=1 superstring where the Lorentz harmonics are used as auxiliary superfields. The incorporation of Lorentz harmonics into the superfield action makes possible to obtain superfield constraints of the induced worldsheet supergravity as equations of motion. Moreover, it becomes evident that a so-called 'Wess-Zumino part' of the superfield action is basically a Lagrangian form of the generalized action principle. We propose to use the second Noether theorem to handle the essential terms in the transformation lows of hidden gauge symmetries, which remove dynamical degrees of freedom from the Lagrange multiplier superfield.

High Energy Physics - TheoryPhysicsPhysics and Astronomy (miscellaneous)WorldsheetLorentz transformationSupergravityHigh Energy Physics::PhenomenologySuperstring theoryEquations of motionFOS: Physical sciencesSuperspaceAction (physics)symbols.namesakeHigh Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)symbolsNoether's theoremMathematical physics
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