Search results for "MONODROMY"

showing 10 items of 44 documents

On coverings with special points and monodromy group a Weyl group of type B_d

2014

In this paper we study Hurwitz spaces parameterizing coverings with special points and with monodromy group a Weyl group of type Bd. We prove that such spaces are irreducible if k > 3d ? 3. Here, k denotes the number of local monodromies that are reflections relative to long roots.

Hurwitz spacespecial fibers branched coveringWeyl groupPure mathematicsGeneral Mathematicsmonodromybraid moves.Type (model theory)Algebrasymbols.namesakeMonodromysymbolsSettore MAT/03 - GeometriaMathematics
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On the irreducibility of Hurwitz spaces of coverings with an arbitrary number of special points

2013

In this paper we study Hurwitz spaces of coverings of Y with an arbitrary number of special points and with monodromy group a Weyl group of type D_d, where Y is a smooth, complex projective curve. We give conditions for which these spaces are irreducible.

Hurwitz spaces Weyl groups special points monodromy braid movesProjective curvePure mathematicsWeyl groupHurwitz quaternionGeneral MathematicsType (model theory)Algebrasymbols.namesakeMonodromyHurwitz's automorphisms theoremsymbolsIrreducibilitySettore MAT/03 - GeometriaMathematics::Representation TheoryMathematicsFilomat
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Integrability Conditions: Recent Results in the Theory of Integrable Models

1990

This paper reports various results achieved recently in the theory of integrable models. These are summarised in the Fig.1! At the Chester meeting [1] two of the authors were concerned [1] with the local Riemann-Hilbert problem (double-lined box in the centre of Fig.1), its limit as a non-local Riemann-Hilbert problem used to solve classical integrable models in 2+1 dimensions (two space and one time dimensions) [2,3], and the connection of this Riemann-Hilbert problem with Ueno’s [4] Riemann-Hilbert problem associated with the representation of the algebra gl(∞) in terms of Z⊗Z matrices (Z the integers) and the solution of the K-P equations in 2+1. We were also concerned [1] with the const…

Loop (topology)Pure mathematicsIntegrable systemQuantum groupLie algebraMonodromy matrixConnection (algebraic framework)Hopf algebraSymplectic manifoldMathematics
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On proper branched coverings and a question of Vuorinen

2022

We study global injectivity of proper branched coverings from the open Euclidean n$n$-ball onto an open subset of the Euclidean n$n$-space in the case where the branch set is compact. In particular, we show that such mappings are homeomorphisms when n=3$n=3$ or when the branch set is empty. This gives a positive answer to the corresponding cases of a question of Vuorinen. Peer reviewed

Mathematics - Complex VariablesGeneral Mathematicseuklidinen geometriaGeometric Topology (math.GT)Euclidean geometryMathematics - Geometric TopologyMAPSFOS: Mathematics111 MathematicsHigh Energy Physics::ExperimentComplex Variables (math.CV)SETMONODROMY57M12 30C65 57M30
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About the role of hamiltonian singularities in controlled systems : applications in quantum mechanics and nonlinear optics

2012

This thesis has two goals: the first one is to improve the control techniques in quantum mechanics, and more specifically in NMR, by using the tools of geometric optimal control. The second one is the study of the influence of Hamiltonian singularities in controlled systems. The chapter about optimal control study three classical problems of NMR : the inversion problem, the influence of the radiation damping term, and the steady state technique. Then, we apply the geometric optimal control to the problem of the population transfert in a three levels quantum system to recover the STIRAP scheme.The two next chapters study Hamiltonian singularities. We show that they allow to control the polar…

Monodromie hamiltonienneNonlinear opticsPolarization attractionContrôle optimal géométrique[ MATH.MATH-GM ] Mathematics [math]/General Mathematics [math.GM][MATH.MATH-GM] Mathematics [math]/General Mathematics [math.GM]Quantum control[ PHYS.COND.CM-GEN ] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Geometric optimal controlHamiltonian singularitiesSingularités hamiltoniennes[MATH.MATH-GM]Mathematics [math]/General Mathematics [math.GM]Optique non-linéaire[PHYS.COND.CM-GEN] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other][PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Attraction de polarisationHamiltonian monodromyContrôle quantique
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MR 3215343 Reviewed Pirola G.P., Rizzi C. and Schlesinger E. A new curve algebraically but not rationally uniformized by radicals. Asian J. Math., 18…

2014

A smooth projective complex curve C is called rationally uniformized by radicals if there exists a covering map C \rightarrow P^1 with solvable Galois group. C is called algebraically uniformized by radicals if there exists a finite covering C^{\prime} \rightarrow C with C^{\prime} rationally uniformized by radicals. Abramovich and Harris posed the following problem in [D. Abramovich and J. Harris, Abelian varieties and curves in $W_{d}(C)$, Compositio Math., 78 (1991), pp. 227–-238]. \vspace{1ex} Statement S(d, h, g): \textit{Suppose C^{\prime} \rightarrow C is a nonconstant map of smooth curves with C of genus g. If C^{\prime} admits a map of degree d or less to a curve of genus h or less…

Monodromy groups Galois groups projective curves.Settore MAT/03 - Geometria
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Quantum spectral curve for arbitrary state/operator in AdS$_5$/CFT$_4$

2015

We give a derivation of quantum spectral curve (QSC) - a finite set of Riemann-Hilbert equations for exact spectrum of planar N=4 SYM theory proposed in our recent paper Phys.Rev.Lett. 112 (2014). We also generalize this construction to all local single trace operators of the theory, in contrast to the TBA-like approaches worked out only for a limited class of states. We reveal a rich algebraic and analytic structure of the QSC in terms of a so called Q-system -- a finite set of Baxter-like Q-functions. This new point of view on the finite size spectral problem is shown to be completely compatible, though in a far from trivial way, with already known exact equations (analytic Y-system/TBA, …

PhysicsHigh Energy Physics - TheoryNuclear and High Energy Physics010308 nuclear & particles physicsOperator (physics)Spectrum (functional analysis)FOS: Physical sciencesMathematical Physics (math-ph)State (functional analysis)AdS-CFT Correspondence01 natural sciencesAdS/CFT correspondenceHigh Energy Physics - Theory (hep-th)MonodromyPhysical Sciences0103 physical sciencesFysikIntegrable Field TheoriesAnti-de Sitter space010306 general physicsFinite setQuantumMathematical PhysicsMathematical physics
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Classical and Quantum Nonultralocal Systems on the Lattice

1997

We classify nonultralocal Poisson brackets for 1-dimensional lattice systems and describe the corresponding regularizations of the Poisson bracket relations for the monodromy matrix. A nonultralocal quantum algebras on the lattices for these systems are constructed. For some class of such algebras an ultralocalization procedure is proposed. The technique of the modified Bethe-Anzatz for these algebras is developed and is applied to the nonlinear sigma model problem.

PhysicsPoisson bracketNonlinear systemPure mathematicsNonlinear Sciences::Exactly Solvable and Integrable SystemsSigma modelPoisson manifoldLattice (order)Quantum mechanicsMonodromy matrixQuantumPoisson algebra
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Nilpotence of orbits under monodromy and the length of Melnikov functions

2021

Abstract Let F ∈ ℂ [ x , y ] be a polynomial, γ ( z ) ∈ π 1 ( F − 1 ( z ) ) a non-trivial cycle in a generic fiber of F and let ω be a polynomial 1-form, thus defining a polynomial deformation d F + e ω = 0 of the integrable foliation given by F . We study different invariants: the orbit depth k , the nilpotence class n , the derivative length d associated with the couple ( F , γ ) . These invariants bind the length l of the first nonzero Melnikov function of the deformation d F + e ω along γ . We analyze the variation of the aforementioned invariants in a simple but informative example, in which the polynomial F is defined by a product of four lines. We study as well the relation of this b…

PhysicsPure mathematicsSequencePolynomialConjectureMelnikov functionAbelian integrals010102 general mathematicsStatistical and Nonlinear PhysicsIterated integralsCondensed Matter Physics01 natural sciencesNilpotence classFoliationDisplacement functionLimit cyclesMonodromySimple (abstract algebra)[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Product (mathematics)0103 physical sciences010307 mathematical physics0101 mathematicsOrbit (control theory)ComputingMilieux_MISCELLANEOUS
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Manifestation of Hamiltonian Monodromy in Nonlinear Wave Systems

2011

International audience; We show that the concept of dynamical monodromy plays a natural fundamental role in the spatiotemporal dynamics of counterpropagating nonlinear wave systems. By means of an adiabatic change of the boundary conditions imposed to the wave system, we show that Hamiltonian monodromy manifests itself through the spontaneous formation of a topological phase singularity (2 - or -phase defect) in the nonlinear waves. This manifestation of dynamical Hamiltonian monodromy is illustrated by generic nonlinear wave models. In particular, we predict that its measurement can be realized in a direct way in the framework of a nonlinear optics experiment.

Physics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]Integrable system010102 general mathematicsGeneral Physics and AstronomyNonlinear opticsPhase singularity01 natural sciencessymbols.namesakeNonlinear systemClassical mechanicsMonodromy0103 physical sciencessymbolsBoundary value problem0101 mathematics010306 general physicsHamiltonian (quantum mechanics)Adiabatic processPhysical Review Letters
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