Search results for "Hamiltonian mechanics"

showing 10 items of 17 documents

Integrability of the one dimensional Schrödinger equation

2018

We present a definition of integrability for the one dimensional Schroedinger equation, which encompasses all known integrable systems, i.e. systems for which the spectrum can be explicitly computed. For this, we introduce the class of rigid functions, built as Liouvillian functions, but containing all solutions of rigid differential operators in the sense of Katz, and a notion of natural boundary conditions. We then make a complete classification of rational integrable potentials. Many new integrable cases are found, some of them physically interesting.

Class (set theory)Integrable systemFOS: Physical sciencesComplex analysisAlgebras01 natural sciencesSchrödinger equationsymbols.namesake[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]0103 physical sciencesBoundary value problem0101 mathematics010306 general physicsGauge field theoryMathematical PhysicsMathematical physicsMathematicsMSC: 34M46 34M50 37J30Liouville equation010102 general mathematicsSpectrum (functional analysis)Operator theory[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Statistical and Nonlinear PhysicsMathematical Physics (math-ph)Differential operatorHamiltonian mechanicssymbols34M46 34M50 37J30
researchProduct

Energy and Personality: A Bridge between Physics and Psychology

2021

[EN] The objective of this paper is to present a mathematical formalism that states a bridge between physics and psychology, concretely between analytical dynamics and personality theory, in order to open new insights in this theory. In this formalism, energy plays a central role. First, the short-term personality dynamics can be measured by the General Factor of Personality (GFP) response to an arbitrary stimulus. This GFP dynamical response is modeled by a stimulus¿response model: an integro-differential equation. The bridge between physics and psychology appears when the stimulus¿response model can be formulated as a linear second order differential equation and, subsequently, reformulat…

Current (mathematics)Differential equationGeneral Mathematics050109 social psychologyStimulus-response modelErmakov–Lewis energy050105 experimental psychologyStimulus (psychology)stimulus–response modelsymbols.namesakeStimulus–response modelQA1-939Computer Science (miscellaneous)0501 psychology and cognitive sciencesEngineering (miscellaneous)Hamiltonian mechanicsPhysicsErmakov-Lewis energyPersonality dynamics05 social sciencesFísicaalgebra_number_theoryAnalytical dynamicsAction (physics)HamiltonianClassical mechanicsMinimum action principlesymbolsGeneral factor of personalityPersonalitatHamiltonian (quantum mechanics)MATEMATICA APLICADAMathematics
researchProduct

An Ecology and Economy Coupling Model. A global stationary state model for a sustainable economy in the Hamiltonian formalism

2020

Abstract The severity of the two deeply correlated crises, the environmental and the economic ones, needs to be faced also in theoretical terms; thus, the authors propose a model yielding a global “stationary state”, following the idea of a “steady-state economics” by Georgescu-Rogen and Herman Daly, by constructing only one dynamical system of ecological and economic coupled variables. This is possible resorting to the generalized Volterra model, that, translated in the Hamiltonian formalism and its Hamilton equations, makes possible to “conjugate” every pair of variables, one economic, the other one ecological, in describing the behavior in time of a unique dynamical system. Applying the …

Economics and Econometrics010504 meteorology & atmospheric sciencesquasiperiodic motionsStability (learning theory)“conjugate” Hamiltonian pairs010501 environmental sciences“Conjugate” Hamiltonian pairsDynamical system01 natural sciencesNewtonian dynamicsVolterra generalized modelsymbols.namesake0105 earth and related environmental sciencesGeneral Environmental ScienceMathematicsUnique dynamical system; Volterra generalized model; “conjugate” Hamiltonian pairs; quasiperiodic motions; Lyapunov stability; global stationary state.Lyapunov stabilityHamiltonian mechanicsQuasi-periodic motionEcologyglobal stationary stateGlobal stationary statePhase spacePath (graph theory)Lyapunov stabilitysymbolsUnique dynamical systemStationary state
researchProduct

Single particle motion in a Penning trap: description in the classical canonical formalism

1992

This paper aims at the development of methods for the calculation of the characteristic frequencies of a Penning trap, taking into account deviations of the actual geometry from the ideal one, anharmonicities of the electric potential, misalignments and inhomogeneities of the magnetic field, additional time dependent electromagnetic fields, and so on. The paper starts by describing the motion of a single charged particle in an ideal hyperbolic Penning trap using the formalism of classical hamiltonian mechanics. The usefulness of rotating coordinates is pointed out, and the importance of conservation of canonical angular momentum is stressed. After transformation to action-angle variables th…

Electromagnetic fieldPhysicsHamiltonian mechanicsAngular momentumCondensed Matter PhysicsPenning trapAtomic and Molecular Physics and OpticsCharged particleMagnetic fieldsymbols.namesakeClassical mechanicssymbolsPhysics::Atomic PhysicsHamiltonian (quantum mechanics)Mathematical PhysicsMagnetosphere particle motionPhysica Scripta
researchProduct

Correlation at low temperature I. Exponential decay

2003

Abstract The present paper generalizes the analysis in (Ann. H. Poincare 1 (2000) 59, Math. J. (AMS) 8 (1997) 123) of the correlations for a lattice system of real-valued spins at low temperature. The Gibbs measure is assumed to be generated by a fairly general Hamiltonian function with pair interaction. The novelty, as compared to [2,20], is that the single-site (self-) energies of the spins are not required to have only a single local minimum and no other extrema. Our derivation of exponential decay of correlations goes through the spectral analysis of a deformed Laplacian closely related to the Witten Laplacian studied in [2,20]. We prove that this Laplacian has a spectral gap above zero…

Hamiltonian mechanicsExponential decay of correlationsSpinsZero (complex analysis)Lattice spin systemsGibbs measuresymbols.namesakeExponential growthQuantum mechanicssymbolsSpectral gapWitten LaplacianGibbs measureExponential decayLaplace operatorAnalysisMathematics
researchProduct

The Poincar\'e-Cartan Form in Superfield Theory

2018

An intrinsic description of the Hamilton-Cartan formalism for first-order Berezinian variational problems determined by a submersion of supermanifolds is given. This is achieved by studying the associated higher-order graded variational problem through the Poincar\'e-Cartan form. Noether theorem and examples from superfield theory and supermechanics are also discussed.

Hamiltonian mechanicsHigh Energy Physics - TheoryMathematics - Differential GeometryPhysics and Astronomy (miscellaneous)BerezinianSuperfieldsymbols.namesakeFormalism (philosophy of mathematics)58E30 46S60 58A20 58J70Poincaré conjectureSupermanifoldsymbolsMathematics::Differential GeometryNoether's theoremMathematical PhysicsMathematical physicsMathematics
researchProduct

The Principles of Canonical Mechanics

2010

Canonical mechanics is a central part of general mechanics, where one goes beyond the somewhat narrow framework of Newtonian mechanics with position coordinates in the three-dimensional space, towards a more general formulation of mechanical systems belonging to a much larger class. This is the first step of abstraction, leaving behind ballistics, satellite orbits, inclined planes, and pendulum-clocks; it leads to a new kind of description that turns out to be useful in areas of physics far beyond mechanics. Through d’Alembert’s principle we discover the concept of the Lagrangian function and the framework of Lagrangian mechanics that is built onto it. Lagrangian functions are particularly …

Hamiltonian mechanicsLegendre transformationsymbols.namesakePoisson bracketPhase spaceLagrangian mechanicssymbolsCanonical transformationMechanicsAnalytical dynamicsHamiltonian systemMathematics
researchProduct

Correlation at Low Temperature: II. Asymptotics

2004

The present paper is a continuation of ref. 4, where the truncated two-point correlation function for a class of lattice spin systems was proved to have exponential decay at low temperature, under a weak coupling assumption. In this paper we compute the asymptotics of the correlation function as the temperature goes to zero. This paper thus extends ref. 3 in two directions: The Hamiltonian function is allowed to have several local minima other than a unique global minimum, and we do not require translation invariance of the Hamiltonian function. We are in particular able to handle spin systems on a general lattice.

Hamiltonian mechanicsMathematical analysisCrystal systemStatistical and Nonlinear PhysicsCorrelationMaxima and minimaContinuationsymbols.namesakeLattice (order)symbolsExponential decayLaplace operatorMathematical PhysicsMathematicsMathematical physicsJournal of Statistical Physics
researchProduct

Spin texture motion in antiferromagnetic and ferromagnetic nanowires

2017

We propose a Hamiltonian dynamics formalism for the current and magnetic field driven dynamics of ferromagnetic and antiferromagnetic domain walls in one dimensional systems. To demonstrate the power of this formalism, we derive Hamilton equations of motion via Poisson brackets based on the Landau-Lifshitz-Gilbert phenomenology, and add dissipative dynamics via the evolution of the energy. We use this approach to study current induced domain wall motion and compute the drift velocity. For the antiferromagnetic case, we show that a nonzero magnetic moment is induced in the domain wall, which indicates that an additional application of a magnetic field would influence the antiferromagnetic do…

Hamiltonian mechanicsPhysicsDrift velocityCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsMagnetic momentFOS: Physical sciences02 engineering and technologyPhysik (inkl. Astronomie)021001 nanoscience & nanotechnology01 natural sciencesMagnetic fieldTransverse planePoisson bracketsymbols.namesakeFerromagnetism0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)symbolsAntiferromagnetismCondensed Matter::Strongly Correlated Electrons010306 general physics0210 nano-technology
researchProduct

A consistent microscopic theory of collective motion in the framework of an ATDHF approach

1978

Based on merely two assumptions, namely the existence of a collective Hamiltonian and that the collective motion evolves along Slater determinants, we first derive a set of adiabatic time-dependent Hartree-Fock equations (ATDHF) which determine the collective path, the mass and the potential, second give a unique procedure for quantizing the resulting classical collective Hamiltonian, and third explain how to use the collective wavefunctions, which are eigenstates of the quantized Hamiltonian.

Hamiltonian mechanicsPhysicsGeneral Physics and AstronomyEigenfunctionAdiabatic theoremsymbols.namesakeClassical mechanicsQuantum mechanicssymbolsSlater determinantMicroscopic theoryAdiabatic processWave functionHamiltonian (quantum mechanics)Annals of Physics
researchProduct