Search results for "Rydberg formula"

showing 10 items of 93 documents

Large numbers of cold positronium atoms created in laser-selected Rydberg states using resonant charge exchange

2016

Lasers are used to control the production of highly excited positronium atoms (Ps*). The laser light excites Cs atoms to Rydberg states that have a large cross section for resonant charge-exchange collisions with cold trapped positrons. For each trial with 30 million trapped positrons, more than 700 000 of the created Ps* have trajectories near the axis of the apparatus, and are detected using Stark ionization. This number of Ps* is 500 times higher than realized in an earlier proof-of-principle demonstration (2004 Phys. Lett. B 597 257). A second charge exchange of these near-axis Ps* with trapped antiprotons could be used to produce cold antihydrogen, and this antihydrogen production is e…

ANTIHYDROGENGeneral PhysicsAntiparticlepositronium0205 Optical Physics0307 Theoretical And Computational ChemistryPLASMASCONFINEMENTPhysics Atomic Molecular & Chemical01 natural sciences010305 fluids & plasmasPositroniumsymbols.namesake0202 Atomic Molecular Nuclear Particle And Plasma PhysicsIonization0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsAntihydrogenpositronsPhysicsCondensed Matter::Quantum GasesScience & TechnologyPhysicsOpticsRydberg statesCondensed Matter PhysicsAtomic and Molecular Physics and Opticscharge-exchangeExcited stateAntimatterPhysical SciencesRydberg formulasymbolsAtomic physicsLepton
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Studies of narrow autoionizing resonances in gadolinium

2003

The autoionization (AI) spectrum of gadolinium between the first and second limits has been investigated by triple-resonance excitation with high-resolution cw lasers. A large number of narrow AI resonances have been observed and assigned total angular momentum J values. The resonances are further divided into members of AI Rydberg series converging to the second limit or other ''interloping'' levels. Fine structure in the Rydberg series has been identified and interpreted in terms of Jc j coupling. A number of detailed studies have been performed on the interloping resonances: These include lifetime determination by lineshape analysis, isotope shifts, hyperfine structure, and photoionizati…

Angular momentumChemistryPhotoionizationAtomic and Molecular Physics and OpticsAnalytical Chemistrysymbols.namesakeAutoionizationTotal angular momentum quantum numberExcited stateRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physicsInstrumentationHyperfine structureSpectroscopyExcitationSpectrochimica Acta Part B: Atomic Spectroscopy
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Rydberg excitation of cold atoms inside a hollow core fiber

2017

We report on a versatile, highly controllable hybrid cold Rydberg atom fiber interface, based on laser cooled atoms transported into a hollow core Kagom\'{e} crystal fiber. Our experiments are the first to demonstrate the feasibility of exciting cold Rydberg atoms inside a hollow core fiber and we study the influence of the fiber on Rydberg electromagnetically induced transparency (EIT) signals. Using a temporally resolved detection method to distinguish between excitation and loss, we observe two different regimes of the Rydberg excitations: one EIT regime and one regime dominated by atom loss. These results are a substantial advancement towards future use of our system for quantum simulat…

Atomic Physics (physics.atom-ph)Electromagnetically induced transparencyFOS: Physical sciencesPhysics::Optics02 engineering and technology01 natural scienceslaw.inventionPhysics - Atomic Physicssymbols.namesakelaw0103 physical sciencesAtomRydberg matterFiberPhysics::Atomic Physics010306 general physicsPhysicsQuantum Physics021001 nanoscience & nanotechnologyLaserRydberg atomRydberg formulasymbolsAtomic physicsQuantum Physics (quant-ph)0210 nano-technologyExcitation
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Narrow-band pulsed electron source based on near-threshold photoionization of Cs in a magneto-optical trap

2019

The newly developed method of time-of-flight (ToF) momentum microscopy was used to analyse the cold electron emission from a Cs 3D magneto-optical trap (MOT). Three-step resonant photoionization was implemented via two intermediate states (6P3/2 pumped with 852 nm laser and 7S1/2 with 1470 nm) and a tuneable femtosecond Ti:sapphire laser for the final ionization step. The magnetic field of the MOT is switched off during the photoionization step. The natural bandwidth of the fs-laser is reduced to 4 meV using optical spectral filters. Precise tuning of the photon energy makes it possible to observe the transition regime between direct photoemission into the open continuum and field induced i…

Atomic Physics (physics.atom-ph)FOS: Physical sciencesPhysics::OpticsElectronPhotoionizationPhoton energy01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmaslaw.inventionsymbols.namesake[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]lawIonizationMagneto-optical trap0103 physical sciencesPhysics::Atomic Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsPhysicsCondensed Matter - Materials Science[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Materials Science (cond-mat.mtrl-sci)Laser3. Good healthFemtosecondRydberg formulasymbolsAtomic physics
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The electronic spectrum of pyrrole

1999

The electronic spectrum of pyrrole has been investigated by performing calculations using a hierarchy of coupled-cluster models consisting of CCS, CC2, CCSD, and CC3. Basis-set effects have been investigated by carrying out calculations using correlation-consistent basis sets augmented with functions especially designed for the description of Rydberg states. Oscillator strengths, excited state dipole moments, and second moments of the electronic charge distributions have been used to characterize the electronic transitions and final states. Structures and vibrational frequencies have been calculated for a few selected states, and the importance of distinguishing between vertical and adiabat…

Basis (linear algebra)ChemistrySpectrum (functional analysis)General Physics and AstronomyElementary chargeDipolesymbols.namesakeAtomic electron transitionExcited stateRydberg formulasymbolsPhysical and Theoretical ChemistryAtomic physicsAdiabatic processThe Journal of Chemical Physics
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A theoretical study of the electronic spectrum of biphenyl

1995

Abstract The electronic spectrum of biphenyl in the energy range up to 6.0 eV has been studied using multiconfigurational second-order perturbation theory (CASPT2) and a basis set of ANO type, including polarization functions on all carbon atoms. The calculated spectrum gives conclusive assignments to all valence excited singlet states and the low-lying triplet states. The change of the torsional angle between the two benzene rings in the different excited states is shown to be of considerable importance and explains the different excitation energies observed in the gas phase as compared to solution or crystalline biphenyl at low temperatures. The intense transition to the 1 1B1u state is m…

BiphenylValence (chemistry)General Physics and AstronomyPolarization (waves)symbols.namesakechemistry.chemical_compoundchemistryExcited stateRydberg formulasymbolsPhysical and Theoretical ChemistryAtomic physicsBenzeneExcitationBasis setChemical Physics Letters
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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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A theoretical study of the electronic spectrum of styrene

1999

Abstract The electronic spectrum of styrene has been studied by using multiconfigurational second-order perturbation theory (CASPT2). The study includes geometry optimization of the ground state, the lowest triplet state, and the lowest singlet excited state. The covalent 2 1 A ′ state placed vertically at 4.34 eV is assigned to the first band. The 1 1 A ′→3 1 A ′ transition located at 4.97 eV is responsible for the second band. The most intense feature involves the 5 1 A ′ state, which is calculated to lie 6.19 eV above the ground state. The lowest singlet–singlet Rydberg transition (3s) is predicted to occur at 5.85 eV.

ChemistryGeneral Physics and AstronomyEnergy minimizationStyrenesymbols.namesakechemistry.chemical_compoundComputer Science::Systems and ControlExcited stateRydberg formulasymbolsSinglet statePhysical and Theoretical ChemistryPerturbation theoryTriplet stateAtomic physicsGround stateChemical Physics Letters
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Vibrational analysis of the electronic spectrum of ethylene based onab initio SCF-CI calculations

1972

Ab initio calculations for CH2 twisting and CC stretching vibrational wavefunctions and energy levels are reported for various electronic states of ethylene C2H4. Electronic transition moments between these states are also obtained to allow a calculation of the oscillator strengths for vibrational transitions involved in various electronic band systems; from this study it is concluded that thevertical electronic energy differenceΔE e may differ significantly from the energy of the absorption maximumΔE max with which it is often equated. In particular it is found in the case of theπ→π * singlet-singlet excitation of ethylene that theΔE e value overestimates the most probable vibrational tran…

ChemistryTransition dipole momentAb initioMolecular electronic transitionsymbols.namesakeAb initio quantum chemistry methodsRydberg formulasymbolsChiropracticsPhysics::Chemical PhysicsPhysical and Theoretical ChemistryAtomic physicsAbsorption (electromagnetic radiation)Wave functionExcitationTheoretica Chimica Acta
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Towards nonlinear optics with cold Rydberg atoms inside a hollow core fiber

2015

We present an experimental setup for studying strongly nonlinear light-matter interactions using cold atoms inside a hollow core fiber. A Rydberg EIT process can potentially be used to generate strong and tunable effective photon-photon interactions.

Condensed Matter::Quantum GasesPhysicsOptical fiberbusiness.industryPhysics::OpticsNonlinear opticslaw.inventionsymbols.namesakelawRydberg atomAtom opticsRydberg formulasymbolsPhysics::Atomic PhysicsFiberCrystal opticsAtomic physicsPhotonicsbusinessCLEO: 2015
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