Search results for "quant-ph"

showing 10 items of 1378 documents

Enabling quantum non-Markovian dynamics by injection of classical colored noise

2017

The non-Markovian nature of quantum systems recently turned to be a key subject for investigations on open quantum system dynamics. Many studies, from its theoretical grounding to its usefulness as a resource for quantum information processing and experimental demonstrations, have been reported in the literature. Typically, in these studies, a structured reservoir is required to make non-Markovian dynamics emerge. Here, we investigate the dynamics of a qubit interacting with a bosonic bath and under the injection of a classical stochastic colored noise. A canonical Lindblad-like master equation for the system is derived by using the stochastic wave function formalism. Then, the non-Markovia…

TRAPPED ATOMSSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciQuantum dynamicsFOS: Physical sciencesMarkov processINFORMAÇÃO QUÂNTICALOCAL OPERATIONS01 natural sciencesSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasSTATE RECOVERYOpen quantum systemsymbols.namesakeTheoretical physics0103 physical sciencesMaster equationCOHERENCEStatistical physics010306 general physicsWave functionQuantumPhysicsQuantum PhysicsOPEN QUANTUM SYSTEMSColors of noiseQubitsymbolsQuantum Physics (quant-ph)
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Longitudinal spin-relaxation in nitrogen-vacancy centers in electron irradiated diamond

2015

We present systematic measurements of longitudinal relaxation rates ($1/T_1$) of spin polarization in the ground state of the nitrogen-vacancy (NV$^-$) color center in synthetic diamond as a function of NV$^-$ concentration and magnetic field $B$. NV$^-$ centers were created by irradiating a Type 1b single-crystal diamond along the [100] axis with 200 keV electrons from a transmission electron microscope with varying doses to achieve spots of different NV$^-$ center concentrations. Values of ($1/T_1$) were measured for each spot as a function of $B$.

TechnologyMaterials sciencePhysics and Astronomy (miscellaneous)Synthetic diamondFOS: Physical sciencesElectronengineering.materiallaw.inventionEngineeringquant-phlawVacancy defectcond-mat.mes-hallMesoscale and Nanoscale Physics (cond-mat.mes-hall)Applied PhysicsQuantum PhysicsCondensed Matter - Materials ScienceCondensed Matter - Mesoscale and Nanoscale PhysicsSpin polarizationRelaxation (NMR)Materials Science (cond-mat.mtrl-sci)Diamondcond-mat.mtrl-sciTransmission electron microscopyPhysical SciencesengineeringAtomic physicsQuantum Physics (quant-ph)Ground stateApplied Physics Letters
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Information dynamics: Temporal behavior of uncertainty measures

2008

We carry out a systematic study of uncertainty measures that are generic to dynamical processes of varied origins, provided they induce suitable continuous probability distributions. The major technical tool are the information theory methods and inequalities satisfied by Fisher and Shannon information measures. We focus on a compatibility of these inequalities with the prescribed (deterministic, random or quantum) temporal behavior of pertinent probability densities.

Theoretical computer science03.65.taComputer sciencesmoluchowski processesQC1-999General Physics and AstronomyFOS: Physical sciencesschrödinger picture evolutionInformation theory05.40.jcfisher informationshannon entropyinformation functionalsQuantumCondensed Matter - Statistical MechanicsMathematical Physicsentropy methodsdynamics of probability densitiesQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)02.50.eyPhysicsMathematical Physics (math-ph)information theoretic inequalitiesCompatibility (mechanics)Probability distributionInformation dynamicsQuantum Physics (quant-ph)
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Supervised learning of time-independent Hamiltonians for gate design

2018

We present a general framework to tackle the problem of finding time-independent dynamics generating target unitary evolutions. We show that this problem is equivalently stated as a set of conditions over the spectrum of the time-independent gate generator, thus transforming the task to an inverse eigenvalue problem. We illustrate our methodology by identifying suitable time-independent generators implementing Toffoli and Fredkin gates without the need for ancillae or effective evolutions. We show how the same conditions can be used to solve the problem numerically, via supervised learning techniques. In turn, this allows us to solve problems that are not amenable, in general, to direct ana…

Theoretical computer scienceDiagonalFOS: Physical sciencesGeneral Physics and AstronomyInverseToffoli gate02 engineering and technologysupervised learning01 natural sciencesUnitary statequantum computingSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasSet (abstract data type)Computer Science::Hardware Architecturesymbols.namesakeComputer Science::Emerging Technologiesquant-ph020204 information systems0103 physical sciences0202 electrical engineering electronic engineering information engineering010306 general physicsEigenvalues and eigenvectorsQuantum computerMathematicsPhysicsFlexibility (engineering)Discrete mathematicsQuantum PhysicsSupervised learningInverse problemHermitian matrixmachine learningQubitsymbolsPairwise comparisonquantum circuitsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Generator (mathematics)Quantum Information and Measurement (QIM) V: Quantum Technologies
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Parametrizations of density matrices

2011

This article gives a brief overview of some recent progress in the characterization and parametrization of density matrices of finite dimensional systems. We discuss in some detail the Bloch-vector and Jarlskog parametrizations and mention briefly the coset parametrization. As applications of the Bloch parametrization we discuss the trace invariants for the case of time dependent Hamiltonians and in some detail the dynamics of three-level systems. Furthermore, the Bloch vector of two-qubit systems as well as the use of the polarization operator basis is indicated. As the main application of the Jarlskog parametrization we construct density matrices for composite systems. In addition, some r…

Theoretical physicsQuantum PhysicsCosetFOS: Physical sciencesQuantum Physics (quant-ph)Atomic and Molecular Physics and Opticsdensity matrixMathematics
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Competition of Direct and Indirect Sources of Thermal Entanglement in a spin star network

2017

A spin star system consisting of three peripheral two-state systems and a central one is considered, with the peripheral spins assumed to interact with each other, as well as with the central one. It is shown that such two couplings, each one being a thermal entanglement source, can significantly compete in the formation of quantum correlations in the thermal state, to the point that they can destroy any thermal entanglement of the peripheral spins.

Thermal entanglementPhysicsStar networkQuantum PhysicsPhysics and Astronomy (miscellaneous)Spinsspin networkFOS: Physical sciencesThermal entanglement01 natural sciencesspin systemSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasQuantum mechanics0103 physical sciencesThermal stateSpin network010306 general physicsQuantum Physics (quant-ph)Nuclear ExperimentQuantumSpin-½
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Rubidium dimers in paraffin-coated cells

2010

Measurements were made to determine the density of rubidium dimer vapor in paraffin-coated cells. The number density of dimers and atoms in similar paraffin-coated and uncoated cells was measured by optical spectroscopy. Due to the relatively low melting point of paraffin, a limited temperature range of 43-80 deg C was explored, with the lower end corresponding to a dimer density of less than 10^7 cm^(-3). With one-minute integration time, a sensitivity to dimer number density of better than 10^6 cm^(-3) was achieved. No significant difference in dimer density was observed between the cells.

Time delay and integrationPhysicsQuantum PhysicsNumber densityAtomic Physics (physics.atom-ph)DimerSignificant differenceAnalytical chemistryGeneral Physics and Astronomychemistry.chemical_elementLow melting pointFOS: Physical sciences02 engineering and technologyAtmospheric temperature range021001 nanoscience & nanotechnology01 natural sciencesPhysics - Atomic PhysicsRubidiumchemistry.chemical_compoundchemistry0103 physical sciences010306 general physics0210 nano-technologySpectroscopyQuantum Physics (quant-ph)
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Ultrarelativistic bound states in the spherical well

2016

We address an eigenvalue problem for the ultrarelativistic (Cauchy) operator $(-\Delta )^{1/2}$, whose action is restricted to functions that vanish beyond the interior of a unit sphere in three spatial dimensions. We provide high accuracy spectral datafor lowest eigenvalues and eigenfunctions of this infinite spherical well problem. Our focus is on radial and orbital shapes of eigenfunctions. The spectrum consists of an ordered set of strictly positive eigenvalues which naturally splits into non-overlapping, orbitally labelled $E_{(k,l)}$ series. For each orbital label $l=0,1,2,...$ the label $k =1,2,...$ enumerates consecutive $l$-th series eigenvalues. Each of them is $2l+1$-degenerate. …

Unit sphereHigh Energy Physics - TheoryFOS: Physical sciences01 natural sciences010305 fluids & plasmasMathematics - Spectral Theory0103 physical sciencesBound stateFOS: Mathematics010306 general physicsSpectral Theory (math.SP)Eigenvalues and eigenvectorsMathematical PhysicsMathematical physicsPhysicsQuantum PhysicsSeries (mathematics)Operator (physics)Spectrum (functional analysis)Cauchy distributionStatistical and Nonlinear PhysicsMathematical Physics (math-ph)EigenfunctionMathematics::Spectral TheoryHigh Energy Physics - Theory (hep-th)Quantum Physics (quant-ph)Journal of Mathematical Physics/ AIP
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On the study of the vibrational energy levels of Arsine molecule

2008

Abstract We compare two formalisms applied to the vibrational modes of the molecule of AsH 3 of C 3 v molecular symmetry group. Indeed, the close stretching modes of this molecule may be considered as those of a three-dimensional oscillator whereas the bending modes may be considered either as a one-dimensional oscillator of symmetry A 1 and a two-dimensional oscillator of symmetry E or as an approximate three-dimensional oscillator. So, we have applied the U ( p  + 1) formalism to the both stretching and bending modes and introduced coupling terms acting on an appropriate coupled vibrational basis through a local mode formalism. We have then compared the result of our fitting with those ob…

Unitary group approachVibrational energy[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]02 engineering and technology01 natural sciencesHot bandchemistry.chemical_compoundArsine[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Normal mode0103 physical sciencesMolecular symmetryMoleculePhysical and Theoretical Chemistry010306 general physicsSpectroscopyPhysicsVibrational excitationsLocal modeNormal mode021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsVibrationchemistryMolecular vibrationAsH3Atomic physics0210 nano-technology
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Spatial correlations of vacuum fluctuations and the Casimir-Polder potential

2003

We calculate the Casimir-Polder intermolecular potential using an effective Hamiltonian recently introduced. We show that the potential can be expressed in terms of the dynamical polarizabilities of the two atoms and the equal-time spatial correlation of the electric field in the vacuum state. This gives support to an interesting physical model recently proposed in the literature, where the potential is obtained from the classical interaction between the instantaneous atomic dipoles induced and correlated by the vacuum fluctuations. Also, the results obtained suggest a more general validity of this intuitive model, for example when external boundaries or thermal fields are present.

Vacuum field fluctuationPhysicsSpatial correlationQuantum PhysicsVacuum stateCasimir forces.General Physics and AstronomyFOS: Physical sciencesSpatial field correlationCasimir effectsymbols.namesakeDipoleQuantum electrodynamicsElectric fieldThermalsymbolsPhysics::Atomic PhysicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Quantum fluctuation
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