Search results for "asma"

showing 10 items of 4204 documents

Theory of warm ionized gases: Equation of state and kinetic Schottky anomaly

2013

Based on accurate Lennard-Jones type interaction potentials, we derive a closed set of state equations for the description of warm atomic gases in the presence of ionization processes. The specific heat is predicted to exhibit peaks in correspondence to single and multiple ionizations. Such kinetic analogue in atomic gases of the Schottky anomaly in solids is enhanced at intermediate and low atomic densities. The case of adiabatic compression of noble gases is analyzed in detail and the implications on sonoluminescence are discussed. In particular, the predicted plasma electron density in a sonoluminescent bubble turns out to be in good agreement with the value measured in recent experiment…

Condensed Matter::Quantum GasesPhysicsEquation of stateBubbleFOS: Physical sciencesKinetic energy01 natural sciences7. Clean energyHeat capacityPhysics - Plasma Physicssingle-bubble sonoluminescence ; plasma ; cavitationCondensed Matter - Other Condensed MatterPlasma Physics (physics.plasm-ph)SonoluminescenceIonization0103 physical sciencesPhysics::Atomic and Molecular ClustersAtomic physics010306 general physicsAdiabatic process010303 astronomy & astrophysicsSchottky anomalyOther Condensed Matter (cond-mat.other)Physical Review E
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Many-body physics with ultracold gases

2007

This article reviews recent experimental and theoretical progress on many-body phenomena in dilute, ultracold gases. Its focus are effects beyond standard weak-coupling descriptions, like the Mott-Hubbard-transition in optical lattices, strongly interacting gases in one and two dimensions or lowest Landau level physics in quasi two-dimensional gases in fast rotation. Strong correlations in fermionic gases are discussed in optical lattices or near Feshbach resonances in the BCS-BEC crossover.

Condensed Matter::Quantum GasesPhysicsHubbard modelCondensed Matter::OtherFOS: Physical sciencesGeneral Physics and AstronomyBCS theoryBose–Hubbard model01 natural sciences010305 fluids & plasmaslaw.inventionCondensed Matter - Other Condensed MatterCoupling (physics)Tonks–Girardeau gas[PHYS.COND.CM-GEN] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]lawUltracold atom[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Quantum mechanicsQuantum electrodynamics0103 physical sciencesAtomtronics010306 general physicsBose–Einstein condensateOther Condensed Matter (cond-mat.other)Reviews of Modern Physics
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EBIT trapping program

1993

The LLNL electron beam ion trap provides the world's only source of stationary highly charged ions up to bare U. This unique capability makes many new atomic and nuclear physics experiments possible.

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsCyclotron resonanceTrappingCondensed Matter PhysicsMass spectrometryAtomic and Molecular Physics and OpticsCharged particleIonNuclear physicsPhysics::Plasma PhysicsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsRadioactive decayElectron ionizationElectron beam ion trapHyperfine Interactions
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Strong enhancement of Penning ionization for asymmetric atom pairs in cold Rydberg gases: the Tom and Jerry effect

2016

We consider Penning ionization of Rydberg atom pairs as an Auger-type process induced by the dipole–dipole interaction and employ semiclassical formulae for dipole transitions to calculate the autoionization width as a function of the principal quantum numbers, n d , n i , of both atoms. While for symmetric atom pairs with the well-known increase of the autoionization width with increasing n 0 is obtained, the result for asymmetric pairs is counterintuitive—for a fixed n i of the ionizing atom of the pair, the autoionization width strongly increases with decreasing n d of the de-excited atom. For H Rydberg atoms this increase reaches two orders of magnitude at the maximum of the n d depende…

Condensed Matter::Quantum GasesPhysicsPhotoionizationCondensed Matter Physics01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmassymbols.namesakeAutoionizationPenning ionizationIonization0103 physical sciencesRydberg atomPrincipal quantum numberPhysics::Atomic and Molecular ClustersRydberg formulasymbolsRydberg matterPhysics::Atomic PhysicsAtomic physics010306 general physicsJournal of Physics B: Atomic, Molecular and Optical Physics
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Instabilities of an electron cloud in a Penning trap

2003

We have measured the storage instabilities of electrons in a Penning trap at low magnetic fields. These measurements are carried out as a function of the trapping voltage, for different magnetic fields. It is seen that these instabilities occur at the same positions when the trapping voltage is expressed as a percentage of the maximum voltage, given by the stability limit. The characteristic frequencies at which these instabilities occur, obey a relation that is given by n zω z + n +ω + + n -ω - = 0, where ω z, ω + and ω - are the axial, perturbed cyclotron and the magnetron frequencies of the trapped electrons respectively, and the n's are integers. The reason for these instabilities are a…

Condensed Matter::Quantum GasesPhysicsPhysics::Atomic PhysicsTrappingPlasmaElectronAtomic physicsPenning trapIon cyclotron resonance spectrometryIon trappingAtomic and Molecular Physics and OpticsIonMagnetic fieldThe European Physical Journal D
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Electron-cooled accumulation of 4 × 109positrons for production and storage of antihydrogen atoms

2016

Four billion positrons (e+) are accumulated in a Penning–Ioffe trap apparatus at 1.2 K and <6 × 10−17 Torr. This is the largest number of positrons ever held in a Penning trap. The e+ are cooled by collisions with trapped electrons (e−) in this first demonstration of using e− for efficient loading of e+ into a Penning trap. The combined low temperature and vacuum pressure provide an environment suitable for antihydrogen () production, and long antimatter storage times, sufficient for high-precision tests of antimatter gravity and of CPT.

Condensed Matter::Quantum GasesPhysicsPhysics::General PhysicsAntiparticleAnnihilationPlasmaElectronCondensed Matter PhysicsPenning trap01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasNuclear physicsTorrAntimatter0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physics010306 general physicsAntihydrogenJournal of Physics B: Atomic, Molecular and Optical Physics
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Rydberg Excitation of a Single Trapped Ion.

2015

We demonstrate excitation of a single trapped cold $^{40}$Ca$^+$ ion to Rydberg levels by laser radiation in the vacuum-ultraviolet at 122 nm wavelength. Observed resonances are identified as 3d$^2$D$_{3/2}$ to 51 F, 52 F and 3d$^2$D$_{5/2}$ to 64F. We model the lineshape and our results imply a large state-dependent coupling to the trapping potential. Rydberg ions are of great interest for future applications in quantum computing and simulation, in which large dipolar interactions are combined with the superb experimental control offered by Paul traps.

Condensed Matter::Quantum GasesPhysicsQuantum PhysicsAtomic Physics (physics.atom-ph)FOS: Physical sciencesGeneral Physics and AstronomyTrappingCoupling (probability)01 natural sciencesIon trappingPhysics - Atomic Physics010305 fluids & plasmasIonsymbols.namesakeDipole0103 physical sciencessymbolsRydberg formulaRydberg matterPhysics::Atomic PhysicsAtomic physicsQuantum Physics (quant-ph)010306 general physicsExcitationPhysical review letters
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van der Waals interactions between excited atoms in generic environments

2015

We consider the the van der Waals force involving excited atoms in general environments, constituted by magnetodielectric bodies. We develop a dynamical approach studying the dynamics of the atoms and the field, mutually coupled. When only one atom is excited, our dynamical theory suggests that for large distances the van der Waals force acting on the ground-state atom is monotonic, while the force acting in the excited atom is spatially oscillating. We show how this latter force can be related to the known oscillating Casimir--Polder force on an excited atom near a (ground-state) body. Our force also reveals a population-induced dynamics: for times much larger that the atomic lifetime the …

Condensed Matter::Quantum GasesPhysicsQuantum PhysicsField (physics)Van der Waals forceVan der Waals strainVan der Waals surfaceFOS: Physical sciencesCasimir-Polder interaction01 natural sciencesLondon dispersion forcestructured environments010305 fluids & plasmassymbols.namesakeExcited state0103 physical sciencesAtomPhysics::Atomic and Molecular ClusterssymbolsVan der Waals radiusPhysics::Atomic Physicsvan der Waals forceAtomic physicsQuantum Physics (quant-ph)010306 general physicsPhysical Review A
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Investigation of Feshbach resonances in ultracold K40 spin mixtures

2017

Magnetically tunable Feshbach resonances are an indispensable tool for experiments with atomic quantum gases. We report on 37 thus far unpublished Feshbach resonances and four further probable Feshbach resonances in spin mixtures of ultracold fermionic $^{40}\mathrm{K}$ with temperatures well below 100 nK. In particular, we locate a broad resonance at $B=389.7\phantom{\rule{0.16em}{0ex}}\text{G}$ with a magnetic width of $26.7\phantom{\rule{0.28em}{0ex}}\text{G}$. Here $1\phantom{\rule{0.28em}{0ex}}\text{G}={10}^{\ensuremath{-}4}\phantom{\rule{0.16em}{0ex}}\text{T}$. Furthermore, by exciting low-energy spin waves, we demonstrate a means to precisely determine the zero crossing of the scatte…

Condensed Matter::Quantum GasesPhysicsQuantum gasResonanceScattering length01 natural sciences010305 fluids & plasmasSpin waveUltracold atom0103 physical sciencesAtomic physics010306 general physicsFeshbach resonanceSpin-½Physical Review A
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2-qubit quantum state transfer in spin chains and cold atoms with weak links

2017

In this paper we discuss the implementation of 2-qubit quantum state transfer (QST) in inhomogeneous spin chains where the sender and the receiver blocks are coupled through the bulk channel via weak links. The fidelity and the typical timescale of the QST are discussed as a function of the parameters of the weak links. Given the possibility of implementing with cold atoms in optical lattices a variety of condensed matter systems, including spin systems, we also discuss the possible implementation of the discussed 2-qubit QST with cold gases with weak links, together with a discussion of the applications and limitations of the presented results.

Condensed Matter::Quantum GasesPhysicsQuantum physiccondensed matterPhysics and Astronomy (miscellaneous)Quantum gasQuantum physicscold atomquantum gaseFunction (mathematics)cold atomsquantum state transfer01 natural sciences010305 fluids & plasmas3. Good healthQubitQuantum mechanics0103 physical sciencesQuantum state transfercold atoms; condensed matter; quantum gases; Quantum physics; quantum state transfer; Physics and Astronomy (miscellaneous)quantum gases010306 general physicsSpin-½
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