Search results for "Equations of motion"

showing 10 items of 143 documents

Slow-roll corrections in multi-field inflation: a separate universes approach

2018

In view of cosmological parameters being measured to ever higher precision, theoretical predictions must also be computed to an equally high level of precision. In this work we investigate the impact on such predictions of relaxing some of the simplifying assumptions often used in these computations. In particular, we investigate the importance of slow-roll corrections in the computation of multi-field inflation observables, such as the amplitude of the scalar spectrum $P_\zeta$, its spectral tilt $n_s$, the tensor-to-scalar ratio $r$ and the non-Gaussianity parameter $f_{NL}$. To this end we use the separate universes approach and $\delta N$ formalism, which allows us to consider slow-roll…

DYNAMICSCosmology and Nongalactic Astrophysics (astro-ph.CO)ComputationFOS: Physical sciencesCMB01 natural sciences114 Physical sciences0103 physical sciencesStatistical physicsinflationMULTICOMPONENT INFLATON010303 astronomy & astrophysicsPhysicsSPECTRUMSlow roll010308 nuclear & particles physicsEquations of motionCONSTRAINTSAstronomy and AstrophysicsObservableCOSMOLOGICAL PERTURBATIONSEXPANSION115 Astronomy Space scienceAmplitudeHypersurfacecosmological perturbation theoryCompact formMulti field2ND-ORDERAPPROXIMATIONGENERATIONAstrophysics - Cosmology and Nongalactic Astrophysics
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Kinetic transport theory with quantum coherence

2008

We derive transport equations for fermions and bosons in spatially or temporally varying backgrounds with special symmetries, by use of the Schwinger-Keldysh formalism. In a noninteracting theory the coherence information is shown to be encoded in new singular shells for the 2-point function. Imposing this phase space structure to the interacting theory leads to a a self-consistent equation of motion for a physcial density matrix, including coherence and a well defined collision integral. The method is applied e.g. to demonstrate how an initially coherent out-of-equlibrium state approaches equlibrium through decoherence and thermalization.

Density matrixPhysicsNuclear and High Energy PhysicsQuantum decoherenceThermal quantum field theory010308 nuclear & particles physicsEquations of motionFOS: Physical sciencesFermion01 natural sciencesHigh Energy Physics - PhenomenologyClassical mechanicsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsPhase space0103 physical sciences010306 general physicsQuantumCoherence (physics)
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High-field nuclear spin relaxation in liquids and solids

1990

The authors generalise the standard theory of nuclear spin relaxation to situations in which the Markovian approximation is not applicable. Expressions for generalised frequency-dependent spin relaxation functions are presented. They show that under high-field conditions the relaxation of longitudinal magnetisation is exponential independent of the particular time dependence of the correlation functions.

Density matrixSpin–spin relaxationMagnetizationCondensed matter physicsChemistrySpin–lattice relaxationEquations of motionRelaxation (physics)Condensed Matter::Strongly Correlated ElectronsGeneral Materials ScienceCondensed Matter PhysicsCole–Cole equationExponential functionJournal of Physics: Condensed Matter
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Time-dependent Landauer-B\"uttiker formalism for superconducting junctions at arbitrary temperatures

2015

We discuss an extension of our earlier work on the time-dependent Landauer--B\"uttiker formalism for noninteracting electronic transport. The formalism can without complication be extended to superconducting central regions since the Green's functions in the Nambu representation satisfy the same equations of motion which, in turn, leads to the same closed expression for the equal-time lesser Green's function, i.e., for the time-dependent reduced one-particle density matrix. We further write the finite-temperature frequency integrals in terms of known special functions thereby considerably speeding up the computation. Numerical simulations in simple normal metal -- superconductor -- normal m…

Density matrixSuperconductivityPhysicsHistoryCondensed Matter - Mesoscale and Nanoscale PhysicsComputationCondensed Matter - SuperconductivityEquations of motionClosed expressionComputer Science ApplicationsEducationSettore FIS/03 - Fisica della MateriaFormalism (philosophy of mathematics)Physics and Astronomy (all)Special functionsQuantum mechanics
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Calculation of size‐intensive transition moments from the coupled cluster singles and doubles linear response function

1994

Coupled cluster singles and doubles linear response (CCLR) calculations have been carried out for excitation energies and dipole transition strengths for the lowest excitations in LiH, CH+, and C4and the results compared with the results from a CI-like approach to equation of motion coupled cluster (EOMCC). The transition strengths are similar in the two approaches for single molecule calculations on small systems. However, the CCLR approach gives size-intensive dipole transition strengths, while title EOMCC formalism does not. Thus, EOMCC calculations can give unphysically dipole transition strengths, e.g., in EOMCC calculations on a sequence of noninteracting LiH systems we obtained a neg…

DipolesGeneral Physics and AstronomySmall systemsExcitation ; Dipoles ; Lithium Hydrides ; Carbynes ; Cations ; Molecular Ions ; Carbon Molecules ; Equations Of Motion ; Correlations ; Response FunctionsPhysics and Astronomy (all)CationsMoleculePhysical and Theoretical Chemistry:FÍSICA::Química física [UNESCO]ExcitationCorrelationsChemistryEquations of motionCarbon MoleculesLinear response functionUNESCO::FÍSICA::Química físicaFormalism (philosophy of mathematics)DipoleCoupled clusterLithium HydridesCarbynesResponse FunctionsAtomic physicsEquations Of MotionMolecular IonsExcitationThe Journal of Chemical Physics
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Random analysis of geometrically non-linear FE modelled structures under seismic actions

1990

Abstract In the framework of the finite element (FE) method, by using the “total Lagrangian approach”, the stochastic analysis of geometrically non-linear structures subjected to seismic inputs is performed. For this purpose the equations of motion are written with the non-linear contribution in an explicit representation, as pseudo-forces, and with the ground motion modelled as a filtered non-stationary white noise Gaussian process, using a Tajimi-Kanai-like filter. Then equations for the moments of the response are obtained by extending the classical Ito's rule to vectors of random processes. The equations of motion, and the equations for moments, obtained here, show a perfect formal simi…

Discrete mathematicsHermite polynomialsSimilarity (geometry)Random excitation; non-linear structuresStochastic processMathematical analysisEquations of motionBuilding and ConstructionWhite noiseFinite element methodRandom excitationNonlinear systemsymbols.namesakesymbolsnon-linear structuresSafety Risk Reliability and QualityGaussian processCivil and Structural EngineeringMathematics
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Stochastic response determination of structural systems modeled via dependent coordinates: a frequency domain treatment based on generalized modal an…

2019

Generalized independent coordinates are typically utilized within an analytical dynamics framework to model the motion of structural and mechanical engineering systems. Nevertheless, for complex systems, such as multi-body structures, an explicit formulation of the equations of motion by utilizing generalized, independent, coordinates can be a daunting task. In this regard, employing a set of redundant coordinates can facilitate the formulation of the governing dynamics equations. In this setting, however, standard response analysis techniques cannot be applied in a straightforward manner. For instance, defining and determining a transfer function within a frequency domain response analysis…

Dynamical systems theoryComputer scienceMechanical EngineeringModal analysisEquations of motion02 engineering and technologyCondensed Matter Physics01 natural sciencesTransfer functionAnalytical dynamicsTransfer function matrixMatrix (mathematics)Power spectral density matrix020303 mechanical engineering & transports0203 mechanical engineeringMechanics of MaterialsFrequency domain0103 physical sciencesAnalytical dynamicApplied mathematicsRandom vibration010301 acousticsSingular matrix
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The electromagnetic and Proca fields revisited: A unified quantization

1997

Quantizing the electromagnetic field with a group formalism faces the difficulty of how to turn the traditional gauge transformation of the vector potential, Aμ(x) → Aμ(x) + ∂μφ(x), into a group law. In this paper, it is shown that the problem can be solved by looking at gauge transformations in a slightly different manner which, in addition, does not require introducing any BRST-like parameter. This gauge transformation does not appear explicitly in the group law of the symmetry but rather as the trajectories associated with generalized equations of motion generated by vector fields with null Noether invariants. In the new approach the parameters of the local group, U(1)(x, t), acquire dyn…

Electromagnetic fieldPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsPhotonQuantization (signal processing)Equations of motionFOS: Physical sciencesAstronomy and AstrophysicsMatemática AplicadaCampos electromagnéticosCampos electromagnéticos ProcaAtomic and Molecular Physics and OpticsCuantización unificadasymbols.namesakeHigh Energy Physics - Theory (hep-th)Proca Cuantización unificadasymbolsVector fieldGauge theoryNoether's theoremMathematical physicsVector potential
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Motion of an electric charge in a terrestrial laboratory.

1995

The equation of motion for a charge in an electromagnetic field is written in the Fermi coordinates of an observer moving with a constant acceleration g=9.8 m/${\mathrm{s}}^{2}$ (${10}^{\mathrm{\ensuremath{-}}18}$ ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$ in units such that c=1). This is involved in the equation of motion not only as a Newtonian term g\ensuremath{\rightarrow}, but also as a relativistic correction of the form ``-2(g\ensuremath{\rightarrow}\ensuremath{\cdot}v\ensuremath{\rightarrow})v\ensuremath{\rightarrow}.'' We have studied the effect of this term under the conditions of an accelerator of particles. To this end, we have considered a constant and uniform magnetic field, a…

Electromagnetic fieldPhysicsLarmor precessionParticle physicsElectric fieldEquations of motionFermi coordinatesCharge (physics)Atomic physicsElectric chargeMagnetic fieldPhysical review. D, Particles and fields
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High order normal form construction near the elliptic orbit of the Sitnikov problem

2011

We consider the Sitnikov problem; from the equations of motion we derive the approximate Hamiltonian flow. Then, we introduce suitable action–angle variables in order to construct a high order normal form of the Hamiltonian. We introduce Birkhoff Cartesian coordinates near the elliptic orbit and we analyze the behavior of the remainder of the normal form. Finally, we derive a kind of local stability estimate in the vicinity of the periodic orbit for exponentially long times using the normal form up to 40th order in Cartesian coordinates.

Elliptic orbitNormal formPerturbation theoryExponential stabilitylaw.inventionsymbols.namesakeExponential stabilitylawCartesian coordinate systemHigh orderRemainderSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsApplied MathematicsMathematical analysisBirkhoff coordinatesEquations of motionAstronomy and AstrophysicsSitnikov problemComputational MathematicsSpace and Planetary ScienceModeling and SimulationSitnikov problemsymbolsBirkhoff coordinates; Exponential stability; Lie-series expansions; Normal form; Perturbation theory; Sitnikov problem; Astronomy and Astrophysics; Space and Planetary ScienceHamiltonian (quantum mechanics)Lie-series expansions
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