Search results for "Normal"

showing 10 items of 2571 documents

Quantum corrections to inflation: the importance of RG-running and choosing the optimal RG-scale

2017

We demonstrate the importance of correctly implementing RG running and choosing the RG scale when calculating quantum corrections to inflaton dynamics. We show that such corrections are negligible for single-field inflation, in the sense of not altering the viable region in the ${n}_{s}\ensuremath{-}r$ plane, when imposing Planck constraints on ${A}_{s}$. Surprisingly, this also applies, in a nontrivial way, for an inflaton coupled to additional spectator degrees of freedom. The result relies on choosing the renormalization scale (pseudo-)optimally, thereby avoiding unphysical large logarithmic corrections to the Friedmann equations and large running of the couplings. We find that the viabl…

Physics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesClassical limitRenormalizationsymbols.namesakeGeneral Relativity and Quantum Cosmologyquantum correctionsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsQuantumMathematical physicsPhysicsta114010308 nuclear & particles physicsFriedmann equationsInflatonRenormalization groupinflatonHigh Energy Physics - Phenomenologysymbols
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Quantum non-Markovianity induced by Anderson localization

2017

As discovered by P. W. Anderson, excitations do not propagate freely in a disordered lattice, but, due to destructive interference, they localise. As a consequence when an atom interacts with a disordered lattice one indeed observes, a non-trivial excitation exchange between atom and lattice. Such non-trivial atomic dynamics will in general be characterised also by a non-trivial quantum information backflow, a clear signature of non-Markovian dynamics. To investigate the above scenario we consider a quantum emitter, or atom, weakly coupled to a uniform coupled-cavity array (CCA). If initially excited, in the absence of disorder, the emitter undergoes a Markovian spontaneous emission by rele…

Physics---Anderson localizationQuantum PhysicsMultidisciplinaryFOS: Physical sciences01 natural sciencesArticleSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasNormal modeExcited stateQuantum mechanics0103 physical sciencesPhenomenological modelAtomSpontaneous emissionQuantum information010306 general physicsQuantum Physics (quant-ph)QuantumScientific Reports
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Frequency Range Selection Method for Vibrational Spectra

2018

Theoretical calculations of vibrational properties are widely used to explain and predict experimental spectra. However, with standard quantum chemical methods all molecular motions are considered, which is rather time-consuming for large molecules. Because typically only a specific spectral region is of experimental interest, we propose here an efficient method that allows calculation of only a selected frequency interval. After a computationally cheap low-level estimate of the molecular motions, the computational time is proportional to the number of normal modes needed to describe this frequency range. Results for a medium-sized molecule show a reduction in computational time of up to 1 …

Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyLetter010304 chemical physics010402 general chemistry01 natural sciencesSpectral line0104 chemical sciencesComputational physicsReduction (complexity)Normal mode0103 physical sciencesRange (statistics)FÍSICO-QUÍMICAMoleculeGeneral Materials ScienceSelection methodSDG 7 - Affordable and Clean EnergyPhysical and Theoretical ChemistryOrder of magnitudeVibrational spectraJournal of Physical Chemistry Letters
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Response functions for infinite fermion systems with velocity dependent interactions

1992

Response functions of infinite Fermi systems are studied in the framework of the self-consistent random phase approximation (RPA). Starting from an effective interaction with velocity and density dependence, or equivalently from a local energy density functional, algebraic expressions for the RPA response function are derived. Simple formulae for the energy-weighted and polarizability sum rules are obtained. The method is illustrated by applications to nuclear matter and liquid 3 He. In nuclear matter, it is shown that existing Skyrme interactions give spin-isospin response functions close to those calculated with finite range interactions. The different renormalization of longitudinal and …

Physics010308 nuclear & particles physicsOscillationNuclear TheoryGeneral Physics and AstronomyFermionNuclear matter01 natural sciencesRenormalizationPolarizabilityQuantum electrodynamicsQuantum mechanics0103 physical sciencesCoulomb010306 general physicsRandom phase approximationEnergy functional
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Numerical integration of subtraction terms

2016

Numerical approaches to higher-order calculations often employ subtraction terms, both for the real emission and the virtual corrections. These subtraction terms have to be added back. In this paper we show that at NLO the real subtraction terms, the virtual subtraction terms, the integral representations of the field renormalisation constants and -- in the case of initial-state partons -- the integral representation for the collinear counterterm can be grouped together to give finite integrals, which can be evaluated numerically. This is useful for an extension towards NNLO.

Physics010308 nuclear & particles physicsSubtractionOrder (ring theory)FOS: Physical sciencesField (mathematics)PartonExtension (predicate logic)01 natural sciencesNumerical integrationRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesApplied mathematicsHardware_ARITHMETICANDLOGICSTRUCTURES010306 general physicsRepresentation (mathematics)
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Eulerian models of the rotating flexible wheelset for high frequency railway dynamics

2019

Abstract In this paper three formulations based on an Eulerian approach are presented to obtain the dynamic response of an elastic solid of revolution, which rotates around its main axis at constant angular velocity. The formulations are especially suitable for the study of the interaction of a solid with a non-rotating structure, such as occurs in the coupled dynamics of a railway wheelset with the track. With respect to previous publications that may adopt similar hypotheses, this paper proposes more compact formulations and eliminates certain numerical problems associated with the presence of second-order derivatives with respect to the spatial coordinates. Three different models are dev…

PhysicsAcoustics and UltrasonicsMechanical EngineeringMathematical analysisRotational symmetryEulerian pathBasis function02 engineering and technologyCondensed Matter Physics01 natural sciencesFinite element methodsymbols.namesake020303 mechanical engineering & transports0203 mechanical engineeringMechanics of MaterialsNormal mode0103 physical sciencessymbolsSolid of revolutionConstant angular velocity010301 acousticsCampbell diagram
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Level statistics and Anderson delocalization in two-dimensional granular materials

2020

Contrary to the theoretical predictions that all waves in two-dimensional disordered materials are localized, Anderson localization is observed only for sufficiently high frequencies in an isotropically jammed two-dimensional disordered granular packing of photoelastic disks. More specifically, we have performed an experiment in analyzing the level statistics of normal mode vibrations. We observe delocalized modes in the low-frequency boson-peak regime and localized modes in the high frequency regime with the crossover frequency just below the Debye frequency. We find that the level-distance distribution obeys Gaussian-Orthogonal-Ensemble (GOE) statistics, i.e. Wigner-Dyson distribution, in…

PhysicsAnderson localizationFOS: Physical sciences02 engineering and technologyCondensed Matter - Soft Condensed Matter021001 nanoscience & nanotechnologyGranular material01 natural sciencesDebye frequencyDelocalized electronNormal mode0103 physical sciencesStatisticsExponentSoft Condensed Matter (cond-mat.soft)010306 general physics0210 nano-technologyScalingAnderson impurity model
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Expressions of Effective Hamiltonian Parameters of XY4 Molecules in the Tetrahedral Formalism

1998

We have derived expressions of second-order effective Hamiltonian parameters of XY4 molecules in the tetrahedral formalism (1992, J. P. Champion et al., "Spectroscopy of the Earth's Atmosphere and Interstellar Medium: Spherical Top Spectra," Academic Press, San Diego). They are written as a function of the force constants of the potential expanded in terms of the dimensionless normal coordinates. These expressions can be used in the isolated band scheme as well as in the polyad one. The ambiguity of the effective Hamiltonian parameters is treated. Relations between the parameters for q2 and q4 terms and Hecht's anharmonicity constants (1960, K. T. Hecht, J. Mol. Spectrosc. 5, 355-389) in th…

PhysicsAnharmonicityAtomic and Molecular Physics and OpticsSpectral lineInterstellar mediumFormalism (philosophy of mathematics)symbols.namesakeQuantum mechanicssymbolsTetrahedronNormal coordinatesPhysical and Theoretical ChemistryHamiltonian (quantum mechanics)SpectroscopyDimensionless quantityJournal of molecular spectroscopy
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Vibrational Energy Levels via Finite-Basis Calculations Using a Quasi-Analytic Form of the Kinetic Energy

2015

A variational method for the calculation of low-lying vibrational energy levels of molecules with small amplitude vibrations is presented. The approach is based on the Watson Hamiltonian in rectilinear normal coordinates and characterized by a quasi-analytic integration over the kinetic energy operator (KEO). The KEO beyond the harmonic approximation is represented by a Taylor series in terms of the rectilinear normal coordinates around the equilibrium configuration. This formulation of the KEO enables its extension to arbitrary order until numerical convergence is reached for those states describing small amplitude motions and suitably represented with a rectilinear system of coordinates. …

PhysicsAnharmonicityKinetic energyComputer Science ApplicationsVibrationNonlinear systemsymbols.namesakeVariational methodClassical mechanicssymbolsTaylor seriesNormal coordinatesPhysical and Theoretical ChemistryHamiltonian (quantum mechanics)Journal of Chemical Theory and Computation
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Examining the N=28 shell closure through high-precision mass measurements of Ar46–48

2020

The strength of the $N=28$ magic number in neutron-rich argon isotopes is examined through high-precision mass measurements of $^{46\text{--}48}\mathrm{Ar}$, performed with the ISOLTRAP mass spectrometer at ISOLDE/CERN. The new mass values are up to 90 times more precise than previous measurements. While they suggest the persistence of the $N=28$ shell closure for argon, we show that this conclusion has to be nuanced in light of the wealth of spectroscopic data and theoretical investigations performed with the SDPF-U phenomenological shell model interaction. Our results are also compared with ab initio calculations using the valence space in-medium similarity renormalization group and the s…

PhysicsArgonValence (chemistry)010308 nuclear & particles physicsSHELL modelchemistry.chemical_elementIsotopes of argonRenormalization groupMass spectrometry01 natural sciencesISOLTRAPchemistryAb initio quantum chemistry methods0103 physical sciencesPhysics::Atomic and Molecular ClustersAtomic physics010306 general physicsPhysical Review C
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