Search results for "ion interactions"

showing 10 items of 15 documents

Full configuration interaction calculation of singlet excited states of Be3

2004

The full configuration interaction (FCI) study of the singlets vertical spectrum of the neutral beryllium trimer has been performed using atomic natural orbitals [3s2p1d] basis set. The FCI triangular equilibrium structure of the ground state has been used to calculate the FCI vertical excitation energies up to 4.8 eV. The FCI vertical ionization potential for the same geometry and basis set amounts to 7.6292 eV. The FCI dipole and quadrupole transition moments from the ground state are reported as well. The FCI electric quadrupole moment of the X (3)A(1) (') ground state has been also calculated with the same basis set (Theta(zz)=-2.6461 a.u., Theta(xx)=Theta(yy)=-1/2Theta(zz)). Twelve of …

Atomic clustersElectron correlationsIonisation potentialGeneral Physics and AstronomyFull configuration interactionBeryllium ; Configuration interactions ; Excited states ; Orbital calculations ; Ground states ; Ionisation potential ; Molecular configurations ; Transition moments ; Quadrupole moments ; Molecular moments ; Electron correlations ; Atomic clustersPhysical and Theoretical Chemistry:FÍSICA::Química física [UNESCO]Basis setElectronic correlationChemistryConfiguration interactionsExcited statesPhysics::Physics EducationMolecular configurationsTransition momentsUNESCO::FÍSICA::Química físicaOrbital calculationsGround statesDipoleExcited stateQuadrupoleQuadrupole momentsMolecular momentsBerylliumAtomic physicsIonization energyGround stateThe Journal of Chemical Physics
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Full configuration interaction calculation of BeH adiabatic states.

2008

An all-electron full configuration interaction (FCI) calculation of the adiabatic potential energy curves of some of the lower states of BeH molecule is presented. A moderately large ANO basis set of atomic natural orbitals (ANO) augmented with Rydberg functions has been used in order to describe the valence and Rydberg states and their interactions. The Rydberg set of ANOs has been placed on the Be at all bond distances. So, the basis set can be described as 4s3p2d1f3s2p1d(BeH)+4s4p2d(Be). The dipole moments of several states and transition dipole strengths from the ground state are also reported as a function of the R(Be-H) distance. The position and the number of states involved in sever…

ChemistryConfiguration interactionsGeneral Physics and AstronomyBond lengthsBeryllium compounds ; Bond lengths ; Configuration interactions ; Ground states ; Molecular moments ; Potential energy surfaces ; Rydberg states ; Vibrational statesRydberg statesPotential energyFull configuration interactionGround statesUNESCO::FÍSICA::Química físicaDipolesymbols.namesakeAtomic orbitalBeryllium compoundsPotential energy surfacesRydberg formulasymbolsMolecular momentsVibrational statesPhysical and Theoretical ChemistryAtomic physicsGround stateAdiabatic process:FÍSICA::Química física [UNESCO]Basis setThe Journal of chemical physics
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Dispersion Interactions between Neutral Atoms and the Quantum Electrodynamical Vacuum

2018

Dispersion interactions are long-range interactions between neutral ground-state atoms or molecules, or polarizable bodies in general, due to their common interaction with the quantum electromagnetic field. They arise from the exchange of virtual photons between the atoms, and, in the case of three or more atoms, are not additive. In this review, after having introduced the relevant coupling schemes and effective Hamiltonians, as well as properties of the vacuum fluctuations, we~outline the main properties of dispersion interactions, both in the nonretarded (van der Waals) and retarded (Casimir--Polder) regime. We then discuss their deep relation with the existence of the vacuum fluctuation…

Electromagnetic fieldHigh Energy Physics - TheoryPhysics and Astronomy (miscellaneous)Field (physics)General MathematicsVan der Waals forceFOS: Physical sciencesVirtual particleCasimir-Polder interactionGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmologyvacuum energyCasimir–Polder interactionssymbols.namesakeMany-body dispersion interactionVacuum energyQuantum mechanics0103 physical sciencesDispersion (optics)Computer Science (miscellaneous)Vacuum fluctuation010306 general physicsvacuum fluctuationsQuantum fluctuationPhysicsQuantum Physics010308 nuclear & particles physicslcsh:Mathematicsmany-body dispersion interactionslcsh:QA1-939Unruh effectHigh Energy Physics - Theory (hep-th)Chemistry (miscellaneous)symbolsvan der Waals forcesvan der Waals forceQuantum Physics (quant-ph)
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Van der Waals and resonance interactions between accelerated atoms in vacuum and the Unruh effect

2017

We discuss different physical effects related to the uniform acceleration of atoms in vacuum, in the framework of quantum electrodynamics. We first investigate the van der Waals/Casimir-Polder dispersion and resonance interactions between two uniformly accelerated atoms in vacuum. We show that the atomic acceleration significantly affects the van der Waals force, yielding a different scaling of the interaction with the interatomic distance and an explicit time dependence of the interaction energy. We argue how these results could allow for an indirect detection of the Unruh effect through dispersion interactions between atoms. We then consider the resonance interaction between two accelerat…

Electromagnetic fieldHistoryField (physics)Vacuum stateFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesResonance (particle physics)General Relativity and Quantum CosmologyEducationsymbols.namesake0103 physical sciencesPhysics::Atomic and Molecular Clusters010306 general physicsQuantum fluctuationPhysicsQuantum Physics010308 nuclear & particles physicsInteraction energyComputer Science ApplicationsUnruh effectsymbolsAtomic physicsvan der Waals forceQuantum Physics (quant-ph)Dispersion Interactions Resonance interactions Vacuum field fluctuations Unruh effect.Journal of Physics: Conference Series
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Detection of the Lowest-Lying Odd-Parity Atomic Levels in Actinium

2020

Two lowest-energy odd-parity atomic levels of actinium, 7s27pP21/2o, 7s27pP23/2o, were observed via two-step resonant laser-ionization spectroscopy and their respective energies were measured to be 7477.36(4) and 12 276.59(2) cm-1. The lifetimes of these states were determined as 668(11) and 255(7) ns, respectively. In addition, we observed the effect of the hyperfine structure on the line for the transition to P23/2o. These properties were calculated using a hybrid approach that combines configuration interaction and coupled-cluster methods, in good agreement with the experiment. The data are of relevance for understanding the complex atomic spectra of actinides and for developing efficien…

FUNDAMENTAL PHYSICSGeneral Physics and Astronomychemistry.chemical_elementHYPERFINE STRUCTURE01 natural sciences7. Clean energyATOMIC SPECTROSCOPYLASER IONIZATION SPECTROSCOPYATOMSCOMPLEX ATOMIC SPECTRALaser coolingIonization0103 physical sciences010306 general physicsSpectroscopyNUMERICAL METHODSHyperfine structurePhysicsHYBRID APPROACHATOM LASERSActinideConfiguration interactionCOUPLED-CLUSTER METHODSACTINIUMMEDICAL ISOTOPE PRODUCTIONActiniumchemistryLASER COOLINGIONIZATIONProduction (computer science)Atomic physicsCONFIGURATION INTERACTIONS
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From small to medium and beyond: a pragmatic approach in predicting properties of Ne containing structures

2013

In this study, we outlined a pragmatic approach for structural studies leading to better understanding of polycarbon structures using 21Ne as a nuclear magnetic resonance (NMR) probe. 21Ne NMR parameters of a single neon atom and its dimer were predicted at the CCSD(T) level in combination with large basis sets. At a lower level of theory, an interaction of neon atom with 1,3-cyclopentadiene ring and with five- and six-membered rings in carbazole was studied using the restricted Hartree–Fock (RHF) and density functional theory (DFT) combined with smaller basis sets. The RHF and DFT modelling of neon interaction with nanosized objects were performed on cyclacenes and selected fullerenes.

Fullerene21Ne NMRDimerBiophysicschemistry.chemical_elementRing (chemistry)Molecular physicsDFTNeonchemistry.chemical_compoundComputational chemistrycarbazoleAtomPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsPhysics::Chemical PhysicsPhysical and Theoretical ChemistryMolecular Biologydispersion interactionsBasis (linear algebra)CarbazolefullerenesCondensed Matter PhysicschemistryDensity functional theorycyclacenesMolecular Physics
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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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Investigating Intermolecular Interactions in a DME-Based Hybrid Ionic Liquid Electrolyte by HOESY NMR

2019

The intermolecular interactions in a hybrid electrolyte based on various compositions of the ionic liquid N-methyl-N-propyl pyrrolidinium bis-fluorosulfonylimide (C3mpyrFSI), LiFSI salt and an ether-based additive, 1,2-dimethoxy ethane (DME), have been investigated using the HOESY (Heteronuclear Overhauser Effect SpectroscopY) NMR experiment. This NMR technique allows a quantification of the intermolecular interactions in ionic liquids (ILs) by measuring the cross-relaxation rate (σ) between different pairs of nuclei. Thereby, we compare the cross-relaxation rates between the cations, anions and DME in these hybrid electrolyte systems using 1H-7Li and 1H-19F HOESY experiments, and interpret…

Ionic bondingSalt (chemistry)02 engineering and technologyElectrolyteNuclear Overhauser effect010402 general chemistry01 natural scienceslcsh:Chemistrychemistry.chemical_compoundComputingMilieux_MISCELLANEOUSOriginal Researchchemistry.chemical_classificationNuclear Overhauser EffectIntermolecular forceSolvationcross-relaxation rates[CHIM.MATE]Chemical Sciences/Material chemistryGeneral Chemistryionic liquid electrolytesion interactions021001 nanoscience & nanotechnology0104 chemical sciencesChemistrychemistryHeteronuclear moleculelcsh:QD1-999Ionic liquidPhysical chemistryHOESY NMR0210 nano-technologyFrontiers in Chemistry
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Dielectron production in proton-proton and proton-lead collisions at √sNN=5.02TeV

2020

The first measurements of dielectron production at midrapidity (|ηe| < 0.8) in proton–proton and proton–lead collisions at √sNN = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT, ee in the ranges mee < 3.5 GeV/c2 and pT, ee < 8 GeV/c, in both collision systems. In proton–proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at √s = 7 and 13 TeV. The slope of the √s dependence of the three measurements is…

Nuclear and High Energy Physics:Kjerne- og elementærpartikkelfysikk: 431 [VDP]ProtonHadronNuclear Theorydielectrondielectron production01 natural sciences7. Clean energyNuclear physicshadron-ion interactionshadron-hadron collisions; dielectron production;Ionic Collisionsdielectron cross sectiondielectron nuclear modification factor0103 physical sciencesInvariant massDielectronCharm (quantum number)Dielectron; hadron-hadron interactions; hadron-ion interactionsPhysics::Atomic PhysicsIonic Collisions; Relativistic Heavy-ion Collisions; Quark-Gluon Plasma010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431hadron-hadron interactionNuclear matterhadron-hadron collisionsNATURAL SCIENCES. Physics.ALICE LHC proton-lead collisions proton-proton collisionsPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431dielectron ; LHC ; dielectron cross section ; dielectron nuclear modification factorQuark–gluon plasmaQuark-Gluon PlasmaHigh Energy Physics::ExperimentLHChadron-hadron interactionsRelativistic Heavy-ion Collisions
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Nonadiabatic orientation, toroidal current, and induced magnetic field in BeO molecules.

2008

It is predicted that oriented BeO molecules would give rise to unprecedentedly strong, unidirectional electric ring current and an associated magnetic field upon excitation by a right or left circularly polarized laser pulse into the first excited degenerate singlet state. The strong toroidal electric ring current of this state is dominated by the ring current of the 1π± orbital about the molecular axis. Our predictions are based on the analysis of the orbital composition of the states involved and are substantiated by high level electronic structure calculations and wavepacket simulations of the laser-driven orientation and excitation dynamics. Luis.Serrano@uv.es

PhotoexcitationToroidMolecular electronic statesMolecule-photon collisionsMagnetic momentChemistryConfiguration interactionsExcited statesGeneral Physics and AstronomyElectronic structureMolecular orientationMagnetic fieldUNESCO::FÍSICA::Química físicaPhotoexcitationCoupled cluster calculationsBeryllium compoundsExcited stateMagnetic momentsPhysical and Theoretical ChemistryAtomic physics:FÍSICA::Química física [UNESCO]Beryllium compounds ; Configuration interactions ; Coupled cluster calculations ; Excited states ; Magnetic moments ; Molecular electronic states ; Molecular orientation ; Molecule-photon collisions ; PhotoexcitationRing currentExcitationThe Journal of chemical physics
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