Search results for "Principal quantum number"

showing 10 items of 31 documents

Location- and observation time-dependent quantum-tunneling

2009

We investigate quantum tunneling in a translation invariant chain of particles. The particles interact harmonically with their nearest neighbors, except for one bond, which is anharmonic. It is described by a symmetric double well potential. In the first step, we show how the anharmonic coordinate can be separated from the normal modes. This yields a Lagrangian which has been used to study quantum dissipation. Elimination of the normal modes leads to a nonlocal action of Caldeira-Leggett type. If the anharmonic bond defect is in the bulk, one arrives at Ohmic damping, i.e. there is a transition of a delocalized bond state to a localized one if the elastic constant exceeds a critical value $…

PhysicsCondensed matter physicsFOS: Physical sciencesDouble-well potentialCondensed Matter PhysicsMagnetic quantum numberElectronic Optical and Magnetic MaterialsCondensed Matter - Other Condensed MatterDelocalized electronNormal modeQuantum mechanicsPrincipal quantum numberRectangular potential barrierQuantum statistical mechanicsQuantum dissipationOther Condensed Matter (cond-mat.other)
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Optomechanical Rydberg-atom excitation via dynamic Casimir-Polder coupling

2014

We study the optomechanical coupling of a oscillating effective mirror with a Rydberg atomic gas, mediated by the dynamical atom-mirror Casimir-Polder force. This coupling may produce a near-field resonant atomic excitation whose probability scales as $\propto (d^2\;a\;n^4\;t)^2/z_0^8$, where $z_0$ is the average atom-surface distance, $d$ the atomic dipole moment, $a$ the mirror's effective oscillation amplitude, $n$ the initial principal quantum number, and $t$ the time. We propose an experimental configuration to realize this system with a cold atom gas trapped at a distance $\sim 2\cdot10 \, \mu$m from a semiconductor substrate, whose dielectric constant is periodically driven by an ext…

CouplingPhysicsCondensed Matter::Quantum GasesQuantum PhysicsRydberg Atoms[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Dynamical Casimir and Casimir-Polder effectGeneral Physics and AstronomyFOS: Physical sciences7. Clean energyQuantum OptomechanicCasimir effectDipolesymbols.namesakeUltracold atomRydberg atomPrincipal quantum numberRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physics[PHYS.COND.CM-SM]Physics [physics]/Condensed Matter [cond-mat]/Statistical Mechanics [cond-mat.stat-mech]Quantum Physics (quant-ph)Excitation
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A note on Δn ≠ 0 Stark transitions in hydrogenlike atoms

1992

In a gaseous helium or hydrogen target slow muons or antiprotons are captured into orbits with a high principal quantum number (n = 15 to 50) to form (μ− α)+ ions, (pα)+ ions, or (pp) atoms respectively. In the subsequent deexcitation process Stark mixing of the intermediary states plays an important role. The successful Mainz Cascade Model assumed Δn = 0 for the Stark transitions, although formally no such selection rule exists. This note examines the reasons why Δn ≠ 0 Stark transitions play only a negligible role in the deexcitation cascade.

PhysicsMuonHydrogenGeneral Physics and Astronomychemistry.chemical_elementIonsymbols.namesakeStark effectchemistryAntiprotonCascadePrincipal quantum numberPhysics::Atomic and Molecular ClusterssymbolsPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentExotic atomAnnalen der Physik
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PROTONIUM: The Mainz Cascade Model

1990

Recent experiments at LEAR have studied extensively the properties of antiprotonic hydrogen, often also called protonium.

PhysicsNuclear physicsHydrogenchemistryCascadeProtoniumPrincipal quantum numberPhysics::Accelerator Physicschemistry.chemical_elementHigh Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment
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Quantum control of ground-state rotational coherence in a linear molecule

2000

We present an experimental and theoretical investigation of the quantum control of ground-state rotational coherence in a linear molecule. A sequence of two temporally separated laser pulses creates a rotational superposition state in ${\mathrm{CO}}_{2}$ whose evolution is monitored through a polarization technique. We study the influence of the phase difference between the two pulses. We show that the overlapping of the two wave packets, produced by each pulse, gives rise to quantum interference that affects the orientational anisotropy of the sample. Because of the large number of coherently excited levels, the interference produces well-separated temporal structures, whose magnitude can …

PhysicsQuantum opticsQuantum phase transitionWAVE-PACKETSTRANSITIONSAtomic and Molecular Physics and OpticsPULSESTIME-RESOLVED DYNAMICSQuantum error correctionExcited stateQuantum mechanicsPrincipal quantum numberINDUCED CONTINUUM STRUCTURECoherent statesIONIZATIONAtomic physicsLASER CONTROLGround stateCoherence (physics)
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Periodic Table of the Elements, History, Education and Evaluation

2021

The periodic tables of transition metal thiophosphates MPS3, transition metal dichalcogenides MX2 and other materials, the origin of chemical elements and toxic trace elements in dried mushrooms are provided. The effective nucleus-electron attraction is proportional to the effective nuclear charge (Zeff) and inversely proportional to the effective principal quantum number (n*). The periodic arch is one of many modern visual displays that have been developed to augment the traditional periodic table of the chemical elements. The table is related to the multiparameter optimisation of N atom, nuclear magnetic resonance and everyday life. Educational activities were developed and evaluated. Se …

PhysicsTrace (linear algebra)Periodic tableTable (information)Effective nuclear chargeIonizaciónlaw.inventionAtomic radiusPeriodic tablelawQuantum mechanicsAtomPrincipal quantum number23 QuímicaTabla periódicaIonization energyIonisationNereis. Interdisciplinary Ibero-American Journal of Methods, Modelling and Simulation.
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Pfaffian and fragmented states atν=52in quantum Hall droplets

2008

When a gas of electrons is confined to two dimensions, application of a strong magnetic field may lead to startling phenomena such as emergence of electron pairing. According to a theory this manifests itself as appearance of the fractional quantum Hall effect with a quantized conductivity at an unusual half-integer v=5/2 Landau level filling. Here we show that similar electron pairing may occur in quantum dots where the gas of electrons is trapped by external electric potentials into small quantum Hall droplets. However, we also find theoretical and experimental evidence that, depending on the shape of the external potential, the paired electron state can break down, which leads to a fragm…

PhysicsCondensed matter physicsQuantum point contactMacroscopic quantum phenomenaQuantum Hall effectCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsElectronic Optical and Magnetic Materialssymbols.namesakePauli exclusion principleQuantum spin Hall effectQuantum mechanicsComposite fermionPrincipal quantum numberFractional quantum Hall effectsymbolsPhysical Review B
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Electronic and magnetic structure of artificial atoms

1999

The concept of shell structure has been found useful in the description of semiconductor quantum dots, which today can be made so small that they contain less than 20 electrons. We review the experimental discovery of magic numbers and spin alignment following Hund’s rules in the addition spectra of vertical quantum dots, and show that these results compare well to model calculations within spin density functional theory. We further discuss the occurrence of spin density waves in quantum dots and quantum wires. For deformable two-dimensional quantum dots (for example, jellium clusters on surfaces), we study the interplay between Hund’s rules and Jahn–Teller deformations and investigate the …

PhysicsQuantum spin Hall effectCondensed matter physicsQuantum dotPrincipal quantum numberQuantum point contactCondensed Matter::Strongly Correlated ElectronsSpin engineeringCondensed Matter::Mesoscopic Systems and Quantum Hall EffectQuantum numberMagnetic quantum numberSpin quantum numberAtomic and Molecular Physics and OpticsThe European Physical Journal D
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Spontaneous emission of a sodium Rydberg atom close to an optical nanofibre

2019

International audience; We report on numerical calculations of the spontaneous emission rate of a Rydberg-excited sodium atom in the vicinity of an optical nanobre. In particular, we study how this rate varies with the distance of the atom to the bre, the bre's radius, the symmetry s or p of the Rydberg state as well as its principal quantum number. We nd that a fraction of the spontaneously emitted light can be captured and guided along the bre. This suggests that such a setup could be used for networking atomic ensembles, manipulated in a collective way due to the Rydberg blockade phenomenon.

FOS: Physical sciences02 engineering and technologyoptical nanofibres01 natural sciencessymbols.namesake020210 optoelectronics & photonics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciencesAtomPrincipal quantum number0202 electrical engineering electronic engineering information engineeringSpontaneous emissionPhysics::Atomic Physics010306 general physicsPhysicsQuantum Physics[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Spontaneous emission ratesRadiusCondensed Matter Physicsspontaneous emission ratesAtomic and Molecular Physics and OpticsSymmetry (physics)Optical nanobresRydberg atomRydberg formulasymbols[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Atomic physicsRydberg stateQuantum Physics (quant-ph)Rydberg atoms
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A weakly-interacting many-body system of Rydberg polaritons based on electromagnetically induced transparency

2020

We proposed utilizing a medium with a high optical depth (OD) and a Rydberg state of low principal quantum number, $n$, to create a weakly-interacting many-body system of Rydberg polaritons, based on the effect of electromagnetically induced transparency (EIT). We experimentally verified the mean field approach to weakly-interacting Rydberg polaritons, and observed the phase shift and attenuation induced by the dipole-dipole interaction (DDI). The DDI-induced phase shift or attenuation can be viewed as a consequence of the elastic or inelastic collisions among the Rydberg polaritons. Using a weakly-interacting system, we further observed that a larger DDI strength caused a width of the mome…

Electromagnetically induced transparencyAtomic Physics (physics.atom-ph)QC1-999Inelastic collisionGeneral Physics and AstronomyFOS: Physical sciencesPhysics::OpticsAstrophysicsPhysics - Atomic Physicssymbols.namesakePrincipal quantum numberBose-Einstein condensation ; room-temperature ; single photons ; thermalization ; optics ; gasPolaritonPhysics::Atomic PhysicsQuantum informationPhysicsCondensed Matter::Quantum GasesQuantum PhysicsCondensed Matter::OtherPhysicsQB460-466Rydberg atomRydberg formulasymbolsRydberg stateAtomic physicsQuantum Physics (quant-ph)
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