Search results for "Matrix"

showing 10 items of 3205 documents

Restrictions for asymmetry and polarizations of recoil in muon capture

1975

Abstract Using the helicity formalism, we discuss muon capture by targets of spin-zero. Owing to the definite neutrino helicity, three independent observables define a complete experiment. The precise relation between asymmetry α and longitudinal polarization P L of recoil, α = 1 + 2 jP L , comes only from rotational invariance. When time-reversal invariance is inserted, there is an additional restriction between the average polarization P av and the longitudinal polarization P L . On the basis of the experimental result P av = 0.43 ± 0.10 for 12 C, we predict P L = −(0.99 +0.01 −0.04 .

PhysicsDensity matrixNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFísicaPolarization (waves)HelicityAsymmetryMuon captureNuclear physicsRecoilRotational invarianceHigh Energy Physics::ExperimentNeutrinomedia_commonNuclear Physics
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Nuclear energy density optimization: Shell structure

2013

Nuclear density functional theory is the only microscopical theory that can be applied throughout the entire nuclear landscape. Its key ingredient is the energy density functional. In this work, we propose a new parameterization UNEDF2 of the Skyrme energy density functional. The functional optimization is carried out using the POUNDerS optimization algorithm within the framework of the Skyrme Hartree-Fock-Bogoliubov theory. Compared to the previous parameterization UNEDF1, restrictions on the tensor term of the energy density have been lifted, yielding a very general form of the energy density functional up to second order in derivatives of the one-body density matrix. In order to impose c…

PhysicsDensity matrixNuclear and High Energy PhysicsWork (thermodynamics)ta114Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsOrbital-free density functional theoryBinding energyNuclear TheoryFOS: Physical sciences01 natural sciencesComputational physicsNuclear physicsNuclear Theory (nucl-th)0103 physical sciencesTensor010306 general physicsParametrizationOpen shellNuclear density
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Gain tuning for continuous-variable quantum teleportation of discrete-variable states

2013

We present a general formalism to describe continuous-variable (CV) quantum teleportation of discrete-variable (DV) states with gain tuning, taking into account experimental imperfections. Here the teleportation output is given by independently transforming each density matrix element of the initial state. This formalism allows us to accurately model various teleportation experiments and to analyze the gain dependence of their respective figures of merit. We apply our formalism to the recent experiment of CV teleportation of qubits [S. Takeda et al., Nature 500, 315 (2013)] and investigate the optimal gain for the transfer fidelity. We also propose and model an experiment for CV teleportati…

PhysicsDensity matrixQuantum PhysicsFOS: Physical sciencesQuantum entanglementQuantum PhysicsQuantum energy teleportationTeleportationAtomic and Molecular Physics and OpticsComputer Science::Emerging TechnologiesSuperdense codingQubitQuantum mechanicsQuantum information scienceQuantum Physics (quant-ph)Quantum teleportation
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Proposal of a Computational Approach for Simulating Thermal Bosonic Fields in Phase Space

2019

When a quantum field is in contact with a thermal bath, the vacuum state of the field may be generalized to a thermal vacuum state, which takes into account the thermal noise. In thermo field dynamics, this is realized by doubling the dimensionality of the Fock space of the system. Interestingly, the representation of thermal noise by means of an augmented space is also found in a distinctly different approach based on the Wigner transform of both the field operators and density matrix, which we pursue here. Specifically, the thermal noise is introduced by augmenting the classical-like Wigner phase space by means of Nos&eacute

PhysicsDensity matrixQuantum PhysicsField (physics)Vacuum statebosonic fieldFOS: Physical sciencesFock spacemolecular dynamics simulationPhase spaceBosonic fieldWigner distribution functionWigner functionStatistical physicsQuantum field theoryWigner function bosonic field temperature control molecular dynamics simulationQuantum Physics (quant-ph)temperature controlPhysics
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The response field and the saddle points of quantum mechanical path integrals

2021

In quantum statistical mechanics, Moyal's equation governs the time evolution of Wigner functions and of more general Weyl symbols that represent the density matrix of arbitrary mixed states. A formal solution to Moyal's equation is given by Marinov's path integral. In this paper we demonstrate that this path integral can be regarded as the natural link between several conceptual, geometric, and dynamical issues in quantum mechanics. A unifying perspective is achieved by highlighting the pivotal role which the response field, one of the integration variables in Marinov's integral, plays for pure states even. The discussion focuses on how the integral's semiclassical approximation relates to…

PhysicsDensity matrixQuantum PhysicsInstanton010308 nuclear & particles physicsInstantonsFOS: Physical sciencesGeneral Physics and AstronomySemiclassical physicsPath integralsResponse field01 natural sciences[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Classical limitsymbols.namesakeClassical mechanics0103 physical sciencesPath integral formulationSaddle point approximationsymbolsDouble-slit experimentFeynman diagramQuantum Physics (quant-ph)010306 general physicsQuantum statistical mechanicsAnnals of Physics
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Misbeliefs and misunderstandings about the non-Markovian dynamics of a damped harmonic oscillator

2003

We use the exact solution for the damped harmonic oscillator to discuss some relevant aspects of its open dynamics often mislead or misunderstood. We compare two different approximations both referred to as Rotating Wave Approximation. Using a specific example, we clarify some issues related to non--Markovian dynamics, non--Lindblad type dynamics, and positivity of the density matrix.

PhysicsDensity matrixQuantum PhysicsPhysics and Astronomy (miscellaneous)Dynamics (mechanics)FOS: Physical sciencesMarkov processType (model theory)Atomic and Molecular Physics and Opticssymbols.namesakeClassical mechanicsExact solutions in general relativitydecoherence non-Markovian dynamics damped harmonicoscillatorsymbolsRotating wave approximationQuantum Physics (quant-ph)Harmonic oscillatorJournal of Optics B: Quantum and Semiclassical Optics
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Limits in the characteristic function description of non-Lindblad-type open quantum systems

2005

In this paper I investigate the usability of the characteristic functions for the description of the dynamics of open quantum systems focussing on non-Lindblad-type master equations. I consider, as an example, a non-Markovian generalized master equation containing a memory kernel which may lead to nonphysical time evolutions characterized by negative values of the density matrix diagonal elements [S.M. Barnett and S. Stenholm, Phys. Rev. A {\bf 64}, 033808 (2001)]. The main result of the paper is to demonstrate that there exist situations in which the symmetrically ordered characteristic function is perfectly well defined while the corresponding density matrix loses positivity. Therefore no…

PhysicsDensity matrixQuantum PhysicsQuantum decoherenceCharacteristic function (probability theory)Stochastic processDiagonalFOS: Physical sciencesAtomic and Molecular Physics and OpticsQuantum mechanicsKernel (statistics)Master equationStatistical physicsQuantum Physics (quant-ph)Quantum
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Estimation of the Repeatedly-Projected Reduced Density Matrix under Decoherence

2007

Decoherence is believed to deteriorate the ability of a purification scheme that is based on the idea of driving a system to a pure state by repeatedly measuring another system in interaction with the former and hinder for a pure state to be extracted asymptotically. Nevertheless, we find a way out of this difficulty by deriving an analytic expression of the reduced density matrix for a two-qubit system immersed in a bath. It is shown that we can still extract a pure state if the environment brings about only dephasing effects. In addition, for a dissipative environment, there is a possibility of obtaining a dominant pure state when we perform a finite number of measurements.

PhysicsDensity matrixQuantum PhysicsQuantum decoherenceSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciAnalytical expressionsDephasingsteFoundations of quantum mechanicFOS: Physical sciencesState (functional analysis)DecoherenceAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaClassical mechanicsDissipative systemReduced density matrixopen systemQuantum Physics (quant-ph)Finite set
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Theoretical gain spectrum of coherently pumped mid-infrared Fabry-Pérot lasers

1992

Abstract We study the gain spectrum of a coherently pumped mid-infrared laser which operates in a linear-cavity (Fabry-Perot), using a three-level density matrix theory. Arbitrary pump and emission field strengths as well as pressure and Doppler broadening are considered. A new strong directional gain asymmetry is found, which is related to the presence of two counterpropagating components in the standing-wave generated field. Gain lineshapes in a wide range of operating conditions are obtained and analysed.

PhysicsDensity matrixRange (particle radiation)Field (physics)business.industrymedia_common.quotation_subjectGainPhysics::OpticsLaserAsymmetryAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticslawElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessFabry–Pérot interferometerDoppler broadeningmedia_commonOptics Communications
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Euclidean random matrix theory: low-frequency non-analyticities and Rayleigh scattering

2011

By calculating all terms of the high-density expansion of the euclidean random matrix theory (up to second-order in the inverse density) for the vibrational spectrum of a topologically disordered system we show that the low-frequency behavior of the self energy is given by $\Sigma(k,z)\propto k^2z^{d/2}$ and not $\Sigma(k,z)\propto k^2z^{(d-2)/2}$, as claimed previously. This implies the presence of Rayleigh scattering and long-time tails of the velocity autocorrelation function of the analogous diffusion problem of the form $Z(t)\propto t^{(d+2)/2}$.

PhysicsDensity matrixStatistical Mechanics (cond-mat.stat-mech)AutocorrelationFOS: Physical sciencesInverseDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural Networks16. Peace & justiceCondensed Matter Physics01 natural sciences010305 fluids & plasmassymbols.namesakeSelf-energyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYQuantum mechanicsPhysical Sciences0103 physical sciencesEuclidean geometrysymbolsRayleigh scatteringDiffusion (business)010306 general physicsRandom matrixCondensed Matter - Statistical MechanicsPhilosophical Magazine
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