Search results for "quant-ph"

showing 10 items of 1378 documents

Imaging the local charge environment of nitrogen-vacancy centers in diamond

2018

Characterizing the local internal environment surrounding solid-state spin defects is crucial to harnessing them as nanoscale sensors of external fields. This is especially germane to the case of defect ensembles which can exhibit a complex interplay between interactions, internal fields and lattice strain. Working with the nitrogen-vacancy (NV) center in diamond, we demonstrate that local electric fields dominate the magnetic resonance behavior of NV ensembles at low magnetic field. We introduce a simple microscopic model that quantitatively captures the observed spectra for samples with NV concentrations spanning over two orders of magnitude. Motivated by this understanding, we propose an…

General PhysicsGeneral Physics and AstronomyFOS: Physical sciences02 engineering and technologyengineering.material01 natural sciencesquant-phElectric fieldVacancy defect0103 physical sciencescond-mat.mes-hallMesoscale and Nanoscale Physics (cond-mat.mes-hall)Diamond cubic010306 general physicsSpin (physics)PhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsDiamondCharge (physics)021001 nanoscience & nanotechnologyDark statePhysical Sciencesengineering0210 nano-technologyQuantum Physics (quant-ph)Order of magnitude
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Approximate energy functionals for one-body reduced density matrix functional theory from many-body perturbation theory

2018

We develop a systematic approach to construct energy functionals of the one-particle reduced density matrix (1RDM) for equilibrium systems at finite temperature. The starting point of our formulation is the grand potential $\Omega [\mathbf{G}]$ regarded as variational functional of the Green's function $G$ based on diagrammatic many-body perturbation theory and for which we consider either the Klein or Luttinger-Ward form. By restricting the input Green's function to be one-to-one related to a set on one-particle reduced density matrices (1RDM) this functional becomes a functional of the 1RDM. To establish the one-to-one mapping we use that, at any finite temperature and for a given 1RDM $\…

Grand potentialSolid-state physicsComplex systemFOS: Physical sciencesdensity matrix functional theory01 natural sciencesCondensed Matter - Strongly Correlated Electronssymbols.namesakePhysics - Chemical Physics0103 physical sciencesSDG 7 - Affordable and Clean Energy010306 general physicsMathematical physicsEnergy functionalChemical Physics (physics.chem-ph)PhysicsQuantum Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyStrongly Correlated Electrons (cond-mat.str-el)010304 chemical physicstiheysfunktionaaliteoriamany-body perturbation theory16. Peace & justiceCondensed Matter PhysicsStationary pointElectronic Optical and Magnetic MaterialsCondensed Matter - Other Condensed Matterapproximate energy functionalssymbolsReduced density matrixapproksimointiQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Ground stateOther Condensed Matter (cond-mat.other)The European Physical Journal B
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On the Study of Resonance Interactions and Splittings in the PH3 Molecule: ν1, ν3, ν2+ν4, and 2ν4 Bands

2002

International audience; The high-resolution (0.005 cm−1) Fourier transform infrared spectrum of PH3 is recorded and analyzed in the region of the fundamental stretching bands, ν1 and ν3. The ν2 + ν4 and 2ν4 bands are taken into account also. Experimental transitions are assigned to the ν1, ν3, ν2 + ν4, and 2ν4 bands with the maximum value of quantum number J equal to 15, 15, 13, and 15, respectively. a1–a2 splittings are observed and described up to the value of quantum number K equal to 10. The analysis of a1/a2 splittings is fulfilled with a Hamiltonian model which takes into account numerous resonance interactions among all the upper vibrational states

Hamiltonian model[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Infrared01 natural sciencessymbols.namesakeNuclear magnetic resonanceVibration–rotation spectra[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciencesMoleculePhysical and Theoretical Chemistry010303 astronomy & astrophysicsSpectroscopy[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]PhysicsResonance interactions010304 chemical physicsResonanceSpectroscopic parametersQuantum numberPH2D moleculeAtomic and Molecular Physics and OpticsFourier transformsymbolsAtomic physicsValue (mathematics)
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A chain of solvable non-Hermitian Hamiltonians constructed by a series of metric operators

2021

We show how, given a non-Hermitian Hamiltonian $H$, we can generate new non-Hermitian operators sequentially, producing a virtually infinite chain of non-Hermitian Hamiltonians which are isospectral to $H$ and $H^\dagger$ and whose eigenvectors we can easily deduce in an almost automatic way; no ingredients are necessary other than $H$ and its eigensystem. To set off the chain and keep it running, we use, for the first time in our knowledge, a series of maps all connected to different metric operators. We show how the procedure works in several physically relevant systems. In particular, we apply our method to various versions of the Hatano-Nelson model and to some PT-symmetric Hamiltonians.

HamiltoniansQuantum PhysicsPure mathematicsSeries (mathematics)010308 nuclear & particles physicsFOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)01 natural sciencesHermitian matrixSet (abstract data type)symbols.namesakeSimilarity mapsIsospectralChain (algebraic topology)0103 physical sciencesMetric (mathematics)symbolsQuantum Physics (quant-ph)010306 general physicsHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaMathematical PhysicsEigenvalues and eigenvectorsMathematicsAnnals of Physics
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The damped harmonic oscillator in deformation quantization

2005

We propose a new approach to the quantization of the damped harmonic oscillator in the framework of deformation quantization. The quantization is performed in the Schr\"{o}dinger picture by a star-product induced by a modified "Poisson bracket". We determine the eigenstates in the damped regime and compute the transition probability between states of the undamped harmonic oscillator after the system was submitted to dissipation.

High Energy Physics - TheoryDeformation quantization[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Canonical quantizationGeneral Physics and AstronomyFOS: Physical sciences01 natural sciences[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]Poisson bracket[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Quantum mechanics0103 physical sciencesdissipative systems010306 general physicsNonlinear Sciences::Pattern Formation and Solitonsquantum mechanics.Harmonic oscillatorEigenvalues and eigenvectorsPhysicsQuantum Physics010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Quantization (signal processing)quantum mechanicsPACS numbers: 03.50.-z 03.50.De 11.10.-z 03.65.DbLandau quantization16. Peace & justiceSecond quantizationClassical mechanicsHigh Energy Physics - Theory (hep-th)Schrödinger pictureQuantum Physics (quant-ph)
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Electromagnetic Duality Anomaly in Curved Spacetimes

2016

The source-free Maxwell action is invariant under electric-magnetic duality rotations in arbitrary spacetimes. This leads to a conserved classical Noether charge. We show that this conservation law is broken at the quantum level in presence of a background classical gravitational field with a non-trivial Chern-Pontryagin invariant, in a parallel way to the chiral anomaly for massless Dirac fermions. Among the physical consequences, the net polarization of the quantum electromagnetic field is not conserved.

High Energy Physics - TheoryElectromagnetic fieldFOS: Physical sciencesGeneral Physics and AstronomyGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmologysymbols.namesakeGravitational field0103 physical sciences010306 general physicsQuantumMathematical PhysicsMathematical physicsPhysicsChiral anomalyQuantum PhysicsConservation law010308 nuclear & particles physicsMathematical Physics (math-ph)Invariant (physics)Classical mechanicsHigh Energy Physics - Theory (hep-th)Dirac fermionsymbolsNoether's theoremQuantum Physics (quant-ph)Physical Review Letters
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Dispersion Interaction between Two Hydrogen Atoms in a Static Electric Field

2019

We consider the dispersion interaction between two ground-state hydrogen atoms, interacting with the quantum electromagnetic field in the vacuum state, in the presence of an external static electric field, both in the nonretarded and in the retarded Casimir-Polder regime. We show that the presence of the external field strongly modifies the dispersion interaction between the atoms, changing its space dependence. Moreover, we find that, for specific geometrical configurations of the two atoms with respect to the external field and/or the relative orientation of the fields acting on the two atoms, it is possible to change the character of the dispersion force, turning it from attractive to re…

High Energy Physics - TheoryElectromagnetic fieldPhysicsQuantum PhysicsCondensed matter physicsVacuum stateFOS: Physical sciencesQuantum fluctuationsGeneral Physics and AstronomySpace (mathematics)Casimir-Polder force01 natural sciencesLondon dispersion forceHigh Energy Physics - Theory (hep-th)Electric field0103 physical sciencesDispersion (optics)Dispersion interactionQuantum Physics (quant-ph)010306 general physicsQuantumQuantum fluctuationPhysical Review Letters
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Vacuum energy densities of a field in a cavity with a mobile boundary

2015

We consider the zero-point field fluctuations, and the related field energy densities, inside a one-dimensional and a three-dimensional cavity with a mobile wall. The mechanical degrees of freedom of the mobile wall are described quantum mechanically and they are fully included in the overall system dynamics. In this optomechanical system, the field and the wall can interact with each other through the radiation pressure on the wall, given by the photons inside the cavity or even by vacuum fluctuations. We consider two cases: the one-dimensional electromagnetic field and the three-dimensional scalar field, and use the Green's functions formalism, which allows extension of the results obtain…

High Energy Physics - TheoryElectromagnetic fieldPhysicsQuantum PhysicsNuclear and High Energy PhysicsPhotonQuantum Optomechanics Vacuum Fluctuations Vacuum Energy DensitiesZero-point energyFOS: Physical sciencesRadiation pressureVacuum energyHigh Energy Physics - Theory (hep-th)Quantum electrodynamicsQuantum Physics (quant-ph)Scalar fieldCavity wallQuantum fluctuation
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Hierarchies of geometric entanglement

2007

We introduce a class of generalized geometric measures of entanglement. For pure quantum states of $N$ elementary subsystems, they are defined as the distances from the sets of $K$-separable states ($K=2,...,N$). The entire set of generalized geometric measures provides a quantification and hierarchical ordering of the different bipartite and multipartite components of the global geometric entanglement, and allows to discriminate among the different contributions. The extended measures are applied to the study of entanglement in different classes of $N$-qubit pure states. These classes include $W$ and $GHZ$ states, and their symmetric superpositions; symmetric multi-magnon states; cluster s…

High Energy Physics - TheoryFOS: Physical sciencesMONOTONESQuantum entanglementSquashed entanglementMultipartite entanglementCombinatoricsSYSTEMSQuantum mechanicsMathematical PhysicsPhysicsQuantum PhysicsQUANTUM-MECHANICSCluster stateCURRENT SITUATIONQUANTUM-MECHANICS CURRENT SITUATION STATES SYSTEMS MONOTONESMathematical Physics (math-ph)Quantum PhysicsAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterMultipartiteHigh Energy Physics - Theory (hep-th)STATESQubitBipartite graphW stateQuantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)Physical Review A
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Strong monogamy of bipartite and genuine multipartite entanglement: The Gaussian case

2007

We demonstrate the existence of general constraints on distributed quantum correlations, which impose a trade-off on bipartite and multipartite entanglement at once. For all N-mode Gaussian states under permutation invariance, we establish exactly a monogamy inequality, stronger than the traditional one, that by recursion defines a proper measure of genuine N-partite entanglement. Strong monogamy holds as well for subsystems of arbitrary size, and the emerging multipartite entanglement measure is found to be scale invariant. We unveil its operational connection with the optimal fidelity of continuous variable teleportation networks.

High Energy Physics - TheoryINFORMATIONGaussianGeneral Physics and AstronomyFOS: Physical sciencesQuantum entanglementSquashed entanglementTeleportationMultipartite entanglementMeasure (mathematics)symbols.namesakeQuantum mechanicsCondensed Matter - Statistical MechanicsMathematical PhysicsMathematicsDiscrete mathematicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Mathematical Physics (math-ph)Quantum PhysicsHigh Energy Physics - Theory (hep-th)symbolsBipartite graphCONTINUOUS-VARIABLE SYSTEMSW stateQuantum Physics (quant-ph)
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