Search results for "35"

showing 10 items of 2413 documents

Irregular Time Dependent Obstacles

2010

Abstract We study the obstacle problem for the Evolutionary p-Laplace Equation when the obstacle is discontinuous and does not have regularity in the time variable. Two quite different procedures yield the same solution.

Yield (engineering)Parabolic obstacle problemVariational inequalities35K55 31B15 31B05Irregular obstacleLeast solutionComputer Science::RoboticsParabolic balayageLavrentiev phenomenonMathematics - Analysis of PDEsSupersolutionp-ParabolicObstacleVariational inequalityObstacle problemFOS: MathematicsApplied mathematicsTime variablePotentialAnalysisAnalysis of PDEs (math.AP)Mathematics
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The Zero Violence Brave Club: A Successful Intervention to Prevent and Address Bullying in Schools

2021

Bullying among peers in schools is a growing problem affecting children and adolescents from an early age worldwide. The consequences of bullying victimization in the emotional development of children and youth and their academic achievement are adverse for them and the rest of the school community, with its negative impact extending into the mid and long run. The Zero Violence Brave Club is implemented in schools in the framework of the Dialogic Model of Violence Prevention, a successful educational action according to the INCLUD-ED project [Strategies for inclusion and social cohesion in Europe from Education] (6th Framework Program of Research of the European Commission). The Zero Violen…

Zero tolerancemedia_common.quotation_subjectPopulationZero Violence Brave ClubRC435-571Special needsComunicació en l'educacióComunicació en treball socialsuccessful educational action03 medical and health sciences0302 clinical medicineBullying in schools0501 psychology and cognitive scienceseducationbystanderOriginal Researchmedia_commonPsychiatryeducation.field_of_studyAssetjament escolar05 social sciencesMental healthPsychiatry and Mental healthFriendshipEducació PrevisióCommunication in social workfriendshipCommunication in educationbullying preventionClubPsychologybreak the silenceSocial psychologyInclusion (education)mental health030217 neurology & neurosurgery050104 developmental & child psychologyQualitative research
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On codimension two embeddings up to link-homotopy

2017

We consider knotted annuli in 4-space, called 2-string-links, which are knotted surfaces in codimension two that are naturally related, via closure operations, to both 2-links and 2-torus links. We classify 2-string-links up to link-homotopy by means of a 4-dimensional version of Milnor invariants. The key to our proof is that any 2-string link is link-homotopic to a ribbon one; this allows to use the homotopy classification obtained in the ribbon case by P. Bellingeri and the authors. Along the way, we give a Roseman-type result for immersed surfaces in 4-space. We also discuss the case of ribbon k-string links, for $k\geq 3$.

[ MATH.MATH-GT ] Mathematics [math]/Geometric Topology [math.GT]Pure mathematicsHomotopy010102 general mathematicsClosure (topology)Geometric Topology (math.GT)CodimensionMSC: 57Q45 (primary); 57M27; 57Q35 (secondary)01 natural sciencesMathematics::Geometric TopologyMathematics - Geometric Topology[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT]0103 physical sciencesRibbonKey (cryptography)FOS: Mathematics010307 mathematical physicsGeometry and Topology0101 mathematicsLink (knot theory)Mathematics
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A note on the Lawrence-Krammer-Bigelow representation

2002

A very popular problem on braid groups has recently been solved by Bigelow and Krammer, namely, they have found a faithful linear representation for the braid group B_n. In their papers, Bigelow and Krammer suggested that their representation is the monodromy representation of a certain fibration. Our goal in this paper is to understand this monodromy representation using standard tools from the theory of hyperplane arrangements. In particular, we prove that the representation of Bigelow and Krammer is a sub-representation of the monodromy representation which we consider, but that it cannot be the whole representation.

[ MATH.MATH-GT ] Mathematics [math]/Geometric Topology [math.GT]Pure mathematicsLinear representation[ MATH.MATH-GR ] Mathematics [math]/Group Theory [math.GR]Braid group20F36Group Theory (math.GR)52C3001 natural sciences[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]52C35Mathematics - Geometric TopologyMathematics::Group TheoryMathematics::Algebraic Geometry[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT]0103 physical sciencesFOS: Mathematics20F36 52C35 52C30 32S22braid groups0101 mathematicsMathematics::Representation TheoryComputingMilieux_MISCELLANEOUSMathematics[MATH.MATH-GT] Mathematics [math]/Geometric Topology [math.GT][MATH.MATH-GR] Mathematics [math]/Group Theory [math.GR]linear representations010102 general mathematicsRepresentation (systemics)FibrationSalvetti complexesGeometric Topology (math.GT)Mathematics::Geometric TopologyHyperplaneMonodromy010307 mathematical physicsGeometry and TopologyMathematics - Group Theory32S22
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La théorie des lignes parallèles de Johann Heinrich Lambert

2014

International audience; The memoir "Theory of parallel lines" (1766) by Johannes Heinrich Lambert is one of the founding texts of hyperbolic geometry, even though his author conceived it as an attempt to show that this geometry does not exist. In fact, Lambert developed that theory with the hope of finding a contradiction. In doing so, he obtained several fundamental results of hyperbolic geometry. This was sixty years before the first writings of Lobachevsky and Bolyai appeared in print. This book contains the first complete translation of Lambert's memoir as well as mathematical and historical commentaries.

[ MATH.MATH-GT ] Mathematics [math]/Geometric Topology [math.GT]géométrie sphérique01-00; 01-02; 01A50 ; 53-02 ; 53-03 ; 53A05 ; 53A35.Lambertspherical geometry[ MATH.MATH-HO ] Mathematics [math]/History and Overview [math.HO]hyperbolic geometryparallèlesgéométrie hyperbolique[MATH.MATH-HO]Mathematics [math]/History and Overview [math.HO][MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT][MATH.MATH-HO] Mathematics [math]/History and Overview [math.HO]parallel lines.parallel lines[MATH.MATH-GT] Mathematics [math]/Geometric Topology [math.GT]
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$PT$-symmetry and Schrödinger operators. The double well case

2016

International audience; We study a class of $PT$-symmetric semiclassical Schrodinger operators, which are perturbations of a selfadjoint one. Here, we treat the case where the unperturbed operator has a double-well potential. In the simple well case, two of the authors have proved in [6] that, when the potential is analytic, the eigenvalues stay real for a perturbation of size $O(1)$. We show here, in the double-well case, that the eigenvalues stay real only for exponentially small perturbations, then bifurcate into the complex domain when the perturbation increases and we get precise asymptotic expansions. The proof uses complex WKB-analysis, leading to a fairly explicit quantization condi…

[ MATH.MATH-SP ] Mathematics [math]/Spectral Theory [math.SP]MSC: 35P20 81Q12 81Q20 35Q40Complex WKB analysis[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]EigenvaluesMathematics::Spectral TheoryPT-symmetryMathematics - Spectral Theory[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]35P20 35Q40 81Q12 81Q20Quantization conditonSchrödinger operatorsMathematical Physics[MATH.MATH-SP]Mathematics [math]/Spectral Theory [math.SP]
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Fractal Weyl law for open quantum chaotic maps

2014

We study the semiclassical quantization of Poincar\'e maps arising in scattering problems with fractal hyperbolic trapped sets. The main application is the proof of a fractal Weyl upper bound for the number of resonances/scattering poles in small domains near the real axis. This result encompasses the case of several convex (hard) obstacles satisfying a no-eclipse condition.

[ NLIN.NLIN-CD ] Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD][PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]FOS: Physical sciencesSemiclassical physicsDynamical Systems (math.DS)35B34 37D20 81Q50 81U05Upper and lower boundsMSC: 35B34 37D20 81Q50 81U05Fractal Weyl lawQuantization (physics)Mathematics - Analysis of PDEs[ MATH.MATH-AP ] Mathematics [math]/Analysis of PDEs [math.AP]Mathematics (miscellaneous)Fractal[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]FOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Mathematics - Dynamical SystemsQuantumMathematical physicsMathematicsScattering[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences - Chaotic DynamicsWeyl lawResonancesQuantum chaotic scattering[NLIN.NLIN-CD]Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD][ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]Chaotic Dynamics (nlin.CD)Statistics Probability and UncertaintyOpen quantum mapComplex planeAnalysis of PDEs (math.AP)Annals of Mathematics
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Hyperfine Paschen-Back regime realized in Rb nanocell

2012

A simple and efficient scheme based on one-dimensional nanometric thin cell filled with Rb and strong permanent ring magnets allowed direct observation of hyperfine Paschen-Back regime on D1 line in 0.5 - 0.7 T magnetic field. Experimental results are perfectly consistent with the theory. In particular, with sigma+ laser excitation, the slopes of B-field dependence of frequency shift for all the 10 individual transitions of 85,87Rb are the same and equal to 18.6 MHz/mT. Possible applications for magnetometry with submicron spatial resolution and tunable atomic frequency references are discussed.

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Atomic Physics (physics.atom-ph)MagnetometerFOS: Physical sciences01 natural sciencesPhysics - Atomic Physicslaw.invention010309 optics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]law0103 physical sciencesOCIS codes: 020.1335 300.6360010306 general physicsHyperfine structure[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]Line (formation)PhysicsNanocellLaserRubidiumAtomic and Molecular Physics and OpticsMagnetic fieldnanocellMagnetHyperfineAtomic physicsPaschen-BackExcitation
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Can there be a general nonlinear PDE theory for existence of solutions ?

2010

Updated version of the 2004 paper arxiv:math/0407026; Contrary to widespread perception, there is ever since 1994 a unified, general type independent theory for the existence of solutions for very large classes of nonlinear systems of PDEs. This solution method is based on the Dedekind order completion of suitable spaces of piece-wise smooth functions on the Euclidean domains of definition of the respective PDEs. The method can also deal with associated initial and/or boundary value problems. The solutions obtained can be assimilated with usual measurable functions or even with Hausdorff continuous functions on the respective Euclidean domains. It is important to note that the use of the or…

[MATH.MATH-GM]Mathematics [math]/General Mathematics [math.GM]MSC 35[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph][MATH.MATH-FA] Mathematics [math]/Functional Analysis [math.FA]QA Mathematics (General)[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP][MATH.MATH-GM] Mathematics [math]/General Mathematics [math.GM][MATH.MATH-AP] Mathematics [math]/Analysis of PDEs [math.AP][PHYS.MPHY] Physics [physics]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-FA]Mathematics [math]/Functional Analysis [math.FA]
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An attempt to classification of the quasi rational solutions to the NLS equation

2015

Based on a representation in terms of determinants of order 2N , an attempt to classification of quasi rational solutions to the one dimensional focusing nonlinear Schrödinger equation (NLS) is given and several conjectures about the structure of the solutions are also formulated. These solutions can be written as a product of an exponential depending on t by a quotient of two polynomials of degree N (N + 1) in x and t depending on 2N −2 parameters. It is remarkable to mention that in this representation, when all parameters are equal to 0, we recover the PN breathers.

[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K10 33Q55 4710A- 4735Fg 4754Bd
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