Search results for "QUANTUM MECHANICS"

showing 10 items of 2468 documents

Modeling21Ne NMR parameters for carbon nanosystems

2013

The potential of nuclear magnetic resonance (NMR) technique in probing the structure of porous systems including carbon nanostructures filled with inert gases is analysed theoretically using accurate calculations of neon ((21) Ne) nuclear magnetic shieldings. The CBS estimates of (21) Ne NMR parameters were performed for single atom, its dimer and neon interacting with acetylene, ethylene and 1,3-cyclopentadiene. Several levels of theory including restricted Hartree-Fock (RHF), Moller-Plesset perturbation theory to the second order (MP2), density functional theory (DFT) with van Voorhis and Scuseria's t-dependent gradient-corrected correlation functional (VSXC), coupled cluster with single …

FullereneDimerchemistry.chemical_elementGeneral ChemistryMolecular physicsNeonchemistry.chemical_compoundCoupled clusterchemistryAcetyleneComputational chemistryAtomGeneral Materials ScienceDensity functional theoryPerturbation theory (quantum mechanics)Magnetic Resonance in Chemistry
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Theoretical prediction of the electronic properties of silicon fullerenes

1994

Summary form only given. High symmetry silicon clusters present currently intense interest because of the possibility they present properties similar to those displayed by fullerenes. Thermodynamic studies have shown that the buckminsterfullerene structure of Si6o is much more stable than other suggested structures. We present here a detailed investigation of the structure and electronic properties of silicon cluster analogous to fullerenes. We have made use of AMI method to obtain reliable geometrical parameters. The calculated valence effective Hamiltonian (VEH) electronic structures are used to predict ionization potentials, electron affinities, HOMO-LUMO energy gaps and first allowed tr…

FullereneValence (chemistry)SiliconDopingchemistry.chemical_elementchemistry.chemical_compoundsymbols.namesakeBuckminsterfullerenechemistryChemical physicsIonizationElectron opticsPhysics::Atomic and Molecular ClusterssymbolsAtomic physicsHamiltonian (quantum mechanics)International Conference on Science and Technology of Synthetic Metals
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Teleportation of squeezing: optimization using non-Gaussian resources

2010

We study the continuous-variable quantum teleportation of states, statistical moments of observables, and scale parameters such as squeezing. We investigate the problem both in ideal and imperfect Vaidman-Braunstein-Kimble protocol setups. We show how the teleportation fidelity is maximized and the difference between output and input variances is minimized by using suitably optimized entangled resources. Specifically, we consider the teleportation of coherent squeezed states, exploiting squeezed Bell states as entangled resources. This class of non-Gaussian states includes photon-added and photon-subtracted squeezed states as special cases. At variance with the case of entangled Gaussian re…

GaussianFOS: Physical sciencesQuantum entanglement01 natural sciencesTeleportation010305 fluids & plasmassymbols.namesakeQuantum mechanics0103 physical sciencesStatistical physics010306 general physicsQuantum information sciencePhysicsQuantum PhysicsBell stateCavity quantum electrodynamicsObservableQuantum PhysicsAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MattersymbolsQuantum Physics (quant-ph)Quantum teleportationPhysics - OpticsOther Condensed Matter (cond-mat.other)Optics (physics.optics)
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Tunable non-Gaussian resources for continuous-variable quantum technologies

2013

We introduce and discuss a set of tunable two-mode states of continuous-variable systems, as well as an efficient scheme for their experimental generation. This novel class of tunable entangled resources is defined by a general ansatz depending on two experimentally adjustable parameters. It is very ample and flexible as it encompasses Gaussian as well as non-Gaussian states. The latter include, among others, known states such as squeezed number states and de-Gaussified photon-added and photon-subtracted squeezed states, the latter being the most efficient non-Gaussian resources currently available in the laboratory. Moreover, it contains the classes of squeezed Bell states and even more ge…

GaussianFOS: Physical sciencesTopology01 natural sciencesTeleportation010309 opticssymbols.namesakeQuantum mechanics0103 physical sciencesQuantum information010306 general physicsPhysicsBell stateQuantum PhysicsQuantum PhysicsAtomic and Molecular Physics and OpticsQuantum technologyCondensed Matter - Other Condensed MattersymbolsCoherent statesQuantum Physics (quant-ph)Realization (systems)Quantum teleportationOther Condensed Matter (cond-mat.other)Optics (physics.optics)Physics - Optics
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Introductory Quantum Physics Courses using a LabVIEW multimedia module

2007

We present the development of a LabVIEW multimedia module for introductory Quantum Physics courses and our experience in the use of this application as an educational tool in learning methodologies. The program solves the Time Dependent Schrodinger Equation for arbitrary potentials. We describe the numerical method used for solving this equation, as well as some mathematical tools employed to reduce the calculation time and to obtain more accurate results. As an illustration, we present the evolution of a wave packet for three different potentials: the repulsive barrier potential, the repulsive step potential, and the harmonic oscillator. This application has been successfully integrated in…

General Computer ScienceMultimediaComputer scienceNumerical analysisGeneral EngineeringFinite difference methodPhysics - Physics EducationFOS: Physical sciencesPhysics::Physics Educationcomputer.software_genreEducationSchrödinger equationSolution of Schrödinger equation for a step potentialsymbols.namesakePhysics Education (physics.ed-ph)Quantum mechanicssymbolscomputerHarmonic oscillator
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Calculation of excited-state properties using general coupled-cluster and configuration-interaction models.

2004

Using string-based algorithms excitation energies and analytic first derivatives for excited states have been implemented for general coupled-cluster (CC) models within CC linear-response (LR) theory which is equivalent to the equation-of-motion (EOM) CC approach for these quantities. Transition moments between the ground and excited states are also considered in the framework of linear-response theory. The presented procedures are applicable to both single-reference-type and multireference-type CC wave functions independently of the excitation manifold constituting the cluster operator and the space in which the effective Hamiltonian is diagonalized. The performance of different LR-CC/EOM-…

General Physics and AstronomyConfiguration interactionStationary pointchemistry.chemical_compoundsymbols.namesakeCoupled clusterAcetylenechemistryQuantum mechanicsExcited statesymbolsPhysical and Theoretical ChemistryAtomic physicsWave functionHamiltonian (quantum mechanics)ExcitationThe Journal of chemical physics
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Kondo Resonance in a Mesoscopic Ring Coupled to a Quantum Dot: Exact Results for the Aharonov-Bohm/Casher Effects

2000

We study the persistent currents induced by both the Aharonov-Bohm and Aharonov-Casher effects in a one-dimensional mesoscopic ring coupled to a side-branch quantum dot at Kondo resonance. For privileged values of the Aharonov-Bohm-Casher fluxes, the problem can be mapped onto an integrable model, exactly solvable by a Bethe ansatz. In the case of a pure magnetic Aharonov-Bohm flux, we find that the presence of the quantum dot has no effect on the persistent current. In contrast, the Kondo resonance interferes with the spin-dependent Aharonov-Casher effect to induce a current which, in the strong-coupling limit, is independent of the number of electrons in the ring.

General Physics and AstronomyFOS: Physical sciences02 engineering and technologyElectron01 natural sciencesResonance (particle physics)Bethe ansatzCondensed Matter - Strongly Correlated Electronssymbols.namesakeQuantum mechanics0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)010306 general physicsAharonov–Bohm effectPhysicsMesoscopic physicsCondensed Matter - Mesoscale and Nanoscale PhysicsNonlinear Sciences - Exactly Solvable and Integrable SystemsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Persistent currentQuantum Physics021001 nanoscience & nanotechnologyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectQuantum dotsymbolsKondo effectExactly Solvable and Integrable Systems (nlin.SI)0210 nano-technology
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Non-hermitian operator modelling of basic cancer cell dynamics

2018

We propose a dynamical system of tumor cells proliferation based on operatorial methods. The approach we propose is quantum-like: we use ladder and number operators to describe healthy and tumor cells birth and death, and the evolution is ruled by a non-hermitian Hamiltonian which includes, in a non reversible way, the basic biological mechanisms we consider for the system. We show that this approach is rather efficient in describing some processes of the cells. We further add some medical treatment, described by adding a suitable term in the Hamiltonian, which controls and limits the growth of tumor cells, and we propose an optimal approach to stop, and reverse, this growth.

General Physics and Astronomylcsh:AstrophysicsTumor cells01 natural sciencesArticle010305 fluids & plasmassymbols.namesakeOperatorial models; Schrödinger dynamics; non Hermitian Hamiltonian; Tumoral proliferation modelSchrödinger dynamicParticle number operatorlcsh:QB460-4660103 physical scienceslcsh:Science010306 general physicsSettore MAT/07 - Fisica MatematicaMathematical physicsPhysicsMedical treatmentOperatorial modelOther Quantitative Biology (q-bio.OT)Non hermitian HamiltonianTumoral proliferation modelQuantitative Biology - Other Quantitative Biologylcsh:QC1-999Birth–death processFOS: Biological sciencesSchrödinger dynamicsCancer cellsymbolslcsh:QOperatorial modelsHamiltonian (quantum mechanics)lcsh:PhysicsSelf-adjoint operator
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Dynamical Casimir-Polder force between an excited atom and a conducting wall

2016

We consider the dynamical atom-surface Casimir-Polder force in the non-equilibrium configuration of an atom near a perfectly conducting wall, initially prepared in an excited state with the field in its vacuum state. We evaluate the time-dependent Casimir-Polder force on the atom, and find that it shows an oscillatory behavior from attractive to repulsive both in time and in space. We also investigate the asymptotic behavior in time of the dynamical force and of related local field quantities, showing that the static value of the force, as obtained by a time-independent approach, is recovered for times much larger than the timescale of the atomic self-dressing, but smaller than the atomic d…

General PhysicsField (physics)Vacuum stateNon-equilibrium thermodynamicsFOS: Physical sciences7. Clean energy01 natural sciencesquant-phQuantum mechanics0103 physical sciencesAtomPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsLocal field01 Mathematical SciencesPhysicsdispersion interactionsCondensed Matter::Quantum GasesQuantum Physics02 Physical Sciences010308 nuclear & particles physicsDynamical Casimir effectCasimir effectPotsdam Transfer - Zentrum für Gründung Innovation Wissens- und TechnologietransferExcited stateAtomic physics03 Chemical SciencesQuantum Physics (quant-ph)Radioactive decay
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Symmetry of mass and energy density of quantum vacuum

Mass is an energy form of quantum vacuum in symmetry with diminished energy density of quantum vacuum. Presence of mass diminishes energy density of quantum vacuum respectively to the energy of a given mass. A given particle with a mass diminishes energy density of quantum vacuum, mass-less particle does not diminish energy of quantum vacuum. In order to explain mass of elementary particles this view does not require existence of the hypothetical boson of Higgs.

General Relativity and Quantum CosmologyQC01 Quantum mechanics
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