Search results for " Mathematical"

showing 10 items of 686 documents

Isotropic-nematic interfacial tension of hard and soft rods: Application of advanced grand canonical biased-sampling techniques

2005

Coexistence between the isotropic and the nematic phase in suspensions of rods is studied using grand canonical Monte Carlo simulations with a bias on the nematic order parameter. The biasing scheme makes it possible to estimate the interfacial tension gamma in systems of hard and soft rods. For hard rods with L/D=15, we obtain gamma ~ 1.4 kB T/L^2, with L the rod length, D the rod diameter, T the temperature, and kB the Boltzmann constant. This estimate is in good agreement with theoretical predictions, and the order of magnitude is consistent with experiments.

PhysicsCondensed matter physicsIsotropy: Physics [G04] [Physical chemical mathematical & earth Sciences]FOS: Physical sciencesGeneral Physics and AstronomyBiasingCondensed Matter - Soft Condensed MatterRodCondensed Matter::Soft Condensed MatterSurface tensionsymbols.namesake: Physique [G04] [Physique chimie mathématiques & sciences de la terre]Liquid crystalPhase (matter)Boltzmann constantsymbolsSoft Condensed Matter (cond-mat.soft)Physical and Theoretical ChemistryOrder of magnitudeThe Journal of Chemical Physics
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Simple monoclinic crystal phase in suspensions of hard ellipsoids

2006

We present a computer simulation study on the crystalline phases of hard ellipsoids of revolution. For aspect ratios $\ensuremath{\geqslant}3$ the previously suggested stretched-fcc phase [Frenkel and Mulder, Mol. Phys. 55, 1171 (1985)] is replaced by a different crystalline phase. Its unit cell contains two ellipsoids with unequal orientations. The lattice is simple monoclinic. The angle of inclination of the lattice, $\ensuremath{\beta}$, is a very soft degree of freedom, while the two right angles are stiff. For one particular value of $\ensuremath{\beta}$, the close-packed version of this crystal is a specimen of the family of superdense packings recently reported [Donev et al., Phys. R…

PhysicsCondensed matter physicsMonte Carlo method: Physics [G04] [Physical chemical mathematical & earth Sciences]NucleationRight angleEllipsoidCondensed Matter::Soft Condensed MatterCrystalColloid: Physique [G04] [Physique chimie mathématiques & sciences de la terre]Lattice (order)Statistical physicsMonoclinic crystal systemPhysical Review E
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The Vlasov Limit for a System of Particles which Interact with a Wave Field

2008

In two recent publications [Commun. PDE, vol.22, p.307--335 (1997), Commun. Math. Phys., vol.203, p.1--19 (1999)], A. Komech, M. Kunze and H. Spohn studied the joint dynamics of a classical point particle and a wave type generalization of the Newtonian gravity potential, coupled in a regularized way. In the present paper the many-body dynamics of this model is studied. The Vlasov continuum limit is obtained in form equivalent to a weak law of large numbers. We also establish a central limit theorem for the fluctuations around this limit.

PhysicsContinuum (measurement)Point particle010102 general mathematicsStatistical and Nonlinear Physics16. Peace & justice01 natural sciencesvlasov limitLaw of large numbers[NLIN.NLIN-CD]Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD]0103 physical sciencesNewtonian fluid010307 mathematical physics0101 mathematicsComputingMilieux_MISCELLANEOUSMathematical PhysicsMathematical physicsCentral limit theoremCommunications in Mathematical Physics
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Coupling of heat flux and vortex polarization in superfluid helium

2020

We consider a macroscopic description of the mutual influence between heat flux and vortex polarization in superfluid helium, in which the vortices produce a lateral deviation of the heat flux, and the heat flux produces a lateral drift of vortices. This coupling is a consequence of a microscopic Magnus force and mutual friction force between the vortices and the flow of excitations carrying the heat. We keep track of these effects with simplified macroscopic equations, and we apply them to second sound propagation between rotating concentric cylinders and to spatial distribution of polarization across a rectangular channel with vortices polarized orthogonally to the channel in the presence…

PhysicsFriction force010102 general mathematicsStatistical and Nonlinear PhysicsMechanicsPolarization (waves)01 natural sciencesVortexPhysics::Fluid DynamicsHeat fluxCondensed Matter::Superconductivity0103 physical sciencesSecond soundConcentric cylinder010307 mathematical physicsMagnus effect0101 mathematicsMathematical PhysicsSuperfluid helium-4Journal of Mathematical Physics
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A star-product approach to noncompact Quantum Groups

1995

Using duality and topological theory of well behaved Hopf algebras (as defined in [2]) we construct star-product models of non compact quantum groups from Drinfeld and Reshetikhin standard deformations of enveloping Hopf algebras of simple Lie algebras. Our star-products act not only on coefficient functions of finite-dimensional representations, but actually on all $C^\infty$ functions, and they exist even for non linear (semi-simple) Lie groups.

PhysicsHigh Energy Physics - TheoryPure mathematics[MATH.MATH-RT]Mathematics [math]/Representation Theory [math.RT]010102 general mathematicsLie groupDuality (optimization)Statistical and Nonlinear Physics16. Peace & justiceHopf algebra01 natural sciences[ MATH.MATH-RT ] Mathematics [math]/Representation Theory [math.RT]Nonlinear systemSimple (abstract algebra)Product (mathematics)Mathematics::Quantum Algebra0103 physical sciencesLie algebraMathematics - Quantum Algebra010307 mathematical physics0101 mathematicsQuantumMathematical PhysicsComputingMilieux_MISCELLANEOUS
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A Remark on an Overdetermined Problem in Riemannian Geometry

2016

Let (M, g) be a Riemannian manifold with a distinguished point O and assume that the geodesic distance d from O is an isoparametric function. Let \(\varOmega \subset M\) be a bounded domain, with \(O \in \varOmega \), and consider the problem \(\varDelta _p u = -1\ \mathrm{in}\ \varOmega \) with \(u=0\ \mathrm{on}\ \partial \varOmega \), where \(\varDelta _p\) is the p-Laplacian of g. We prove that if the normal derivative \(\partial _{\nu }u\) of u along the boundary of \(\varOmega \) is a function of d satisfying suitable conditions, then \(\varOmega \) must be a geodesic ball. In particular, our result applies to open balls of \(\mathbb {R}^n\) equipped with a rotationally symmetric metr…

PhysicsIsoparametric functionComparison principleGeodesic010102 general mathematicsRotationally symmetric spacesRiemannian manifoldRiemannian geometry01 natural sciencesRotationally symmetric spaceCombinatoricsOverdetermined systemsymbols.namesakeBounded function0103 physical sciencessymbolsComparison principle; Isoparametric functions; Overdetermined PDE; Riemannian Geometry; Rotationally symmetric spaces; Mathematics (all)Isoparametric functionsMathematics (all)Overdetermined PDEMathematics::Differential Geometry010307 mathematical physics0101 mathematicsRiemannian Geometry
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A note on the Pais-Uhlenbeck model and its coherent states

2011

In some recent papers many quantum aspects of the Pais-Uhlenbeck model were discussed. In particular, several inequivalent hamiltonians have been proposed, with different features, giving rise, at a quantum level, to the fourth-order differential equation of the model. Here we propose two new possible hamiltonians which also produce the same differential equation. In particular our first hamiltonian is self-adjoint and positive. Our second proposal is written in terms of pseudo-bosonic operators. We discuss in details the ground states of these hamiltonians and the (bi-)coherent states of the models.

PhysicsPhysics and Astronomy (miscellaneous)Differential equationGeneral MathematicsQuantum levelsymbols.namesakeQuantum mechanicsCoherent states in mathematical physicssymbolsCoherent statesPseudo-bosonsHamiltonian (quantum mechanics)QuantumCoherent stateSettore MAT/07 - Fisica Matematica
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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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QCD condensates from tau-decay data: A functional approach

2004

We study a functional method to extract the V − A condensate of dimension 6 from a comparison of τ -decay data with the asymptotic space-like QCD prediction. Our result is in agreement within errors with that from conventional analyses based on finite energy sum rules.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsFunctional approachFOS: Physical sciencesPerturbation (Mathematics)Mathematical analysisRenormalization (Physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum mechanics[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quantum chromodynamics -- Mathematical modelsSum rule in quantum mechanicsEnergy (signal processing)
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A calorimeter for the precise determination of the activity of the 144Ce-144Pr anti-neutrino source in the SOX experiment

2018

We describe the design and the performance of a high precision thermal calorimeter, whose purpose was the measurement of the total activity of the 144Ce-144Pr anti-neutrino source of the SOX (Short distance neutrino Oscillation with BoreXino) experiment. SOX aimed at the search for eV-scale sterile neutrinos by means of the Borexino detector at the Laboratori Nazionali del Gran Sasso in Italy and of a very powerful artificial anti-neutrino source located at 8.51 m from the detector center. In order to obtain the required sensitivity, the activity of the source (approximately 150 kCi) had to be known at 1% precision. In this work we report the design of the experimental apparatus and the res…

PhysicsRadiation monitoringPhysics::Instrumentation and Detectors010308 nuclear & particles physicsDetector01 natural sciencesParticle detectorCalorimeterNuclear physicsCalorimetersNeutrino detectorMockup0103 physical sciencesHigh Energy Physics::ExperimentNeutrinoCalorimeters; Radiation monitoring; Instrumentation; Mathematical Physics010306 general physicsNeutrino oscillationInstrumentationMathematical PhysicsBorexinoJournal of Instrumentation
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