Search results for "Plasmas"

showing 10 items of 1475 documents

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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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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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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Breaking of SU(4) symmetry and interplay between strongly correlated phases in the Hubbard model

2016

We study the thermodynamic properties of four-component fermionic mixtures described by the Hubbard model using the dynamical mean-field-theory approach. Special attention is given to the system with SU(4)-symmetric interactions at half filling, where we analyze equilibrium many-body phases and their coexistence regions at nonzero temperature for the case of simple cubic lattice geometry. We also determine the evolution of observables in low-temperature phases while lowering the symmetry of the Hamiltonian towards the two-band Hubbard model. This is achieved by varying interflavor interactions or by introducing the spin-flip term (Hund's coupling). By calculating the entropy for different s…

Condensed Matter::Quantum GasesPhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsFOS: Physical sciencesObservableSimple cubic lattice01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsQuantum Gases (cond-mat.quant-gas)Quantum mechanics0103 physical sciencesHomogeneous spaceCondensed Matter - Quantum Gases010306 general physicsPhysical Review B
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Quantum critical point in a periodic Anderson model

2000

We investigate the symmetric Periodic Anderson Model (PAM) on a three-dimensional cubic lattice with nearest-neighbor hopping and hybridization matrix elements. Using Gutzwiller's variational method and the Hubbard-III approximation (which corresponds to the exact solution of an appropriate Falicov-Kimball model in infinite dimensions) we demonstrate the existence of a quantum critical point at zero temperature. Below a critical value $V_c$ of the hybridization (or above a critical interaction $U_c$) the system is an {\em insulator} in Gutzwiller's and a {\em semi-metal} in Hubbard's approach, whereas above $V_c$ (below $U_c$) it behaves like a metal in both approximations. These prediction…

Condensed Matter::Quantum GasesPhysicsStrongly Correlated Electrons (cond-mat.str-el)Quantum Monte CarloFOS: Physical sciencesCritical value01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityVariational methodQuantum critical pointQuantum mechanics0103 physical sciencesDensity of statesCondensed Matter::Strongly Correlated ElectronsStrongly correlated material010306 general physicsAnderson impurity modelPhysical Review B
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FERMION CONDENSATION, T -LINEAR RESISTIVITY AND PLANCKIAN LIMIT

2019

We explain recent challenging experimental observations of universal scattering rate related to the linear-temperature resistivity exhibited by a large corps of both strongly correlated Fermi systems and conventional metals. We show that the observed scattering rate in strongly correlated Fermi systems like heavy fermion metals and high-$T_c$ superconductors stems from phonon contribution that induce the linear temperature dependence of a resistivity. The above phonons are formed by the presence of flat band, resulting from the topological fermion condensation quantum phase transition (FCQPT). We emphasize that so - called Planckian limit, widely used to explain the above universal scatteri…

Condensed Matter::Quantum GasesPhysicsSuperconductivityQuantum phase transitionQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)Physics and Astronomy (miscellaneous)Condensed matter physicsSolid-state physicsPhononFOS: Physical sciencesFermion01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsElectrical resistivity and conductivityLattice (order)Scattering rate0103 physical sciencesCondensed Matter::Strongly Correlated ElectronsQuantum Physics (quant-ph)010306 general physicsПИСЬМА В ЖУРНАЛ ЭКСПЕРИМЕНТАЛЬНОЙ И ТЕОРЕТИЧЕСКОЙ ФИЗИКИ
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