Search results for "Quantum gas"

showing 10 items of 654 documents

Vacancy-like Dressed States in Topological Waveguide QED

2020

We identify a class of dressed atom-photon states formingat the same energy of the atom at any coupling strength. As a hallmark, their photonic component is an eigenstate of the bare photonic bath with a vacancy in place of the atom. The picture accommodates waveguide-QED phenomena where atoms behave as perfect mirrors, connecting in particular dressed bound states (BS) in the continuum or BIC with geometrically-confined photonic modes. When applied to photonic lattices, the framework provides a general criterion to predict dressed BS in lattices with topological properties by putting them in one-to-one correspondence with photonic BS. New classes of dressed BS are thus predicted in the pho…

---Condensed Matter::Quantum GasesPhysicsQuantum PhysicsWaveguide (electromagnetism)PhotonSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciContinuum (topology)business.industryFOS: Physical sciencesPhysics::OpticsGeneral Physics and Astronomy01 natural sciencesCavity QED Photonic bound states topological latticeVacancy defectQuantum mechanics0103 physical sciencesAtomBound statePhysics::Atomic PhysicsPhotonicsQuantum Physics (quant-ph)010306 general physicsbusinessEigenvalues and eigenvectors
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Work fluctuations in bosonic Josephson junctions

2016

We calculate the first two moments and full probability distribution of the work performed on a system of bosonic particles in a two-mode Bose-Hubbard Hamiltonian when the self-interaction term is varied instantaneously or with a finite-time ramp. In the instantaneous case, we show how the irreversible work scales differently depending on whether the system is driven to the Josephson or Fock regime of the bosonic Josephson junction. In the finite-time case, we use optimal control techniques to substantially decrease the irreversible work to negligible values. Our analysis can be implemented in present-day experiments with ultracold atoms and we show how to relate the work statistics to that…

---Josephson effectPopulationFOS: Physical sciences01 natural sciencesSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasFock spacesymbols.namesakequant-phUltracold atomQuantum mechanics0103 physical sciences010306 general physicseducationPhysicsCondensed Matter::Quantum GasesQuantum Physicseducation.field_of_studyOptimal controlAtomic and Molecular Physics and OpticsQuantum Gases (cond-mat.quant-gas)symbolsProbability distributionCondensed Matter - Quantum GasesHamiltonian (quantum mechanics)Quantum Physics (quant-ph)cond-mat.quant-gas
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Superconducting size effect in thin films under electric field: Mean-field self-consistent model

2019

We consider effects of an externally applied electrostatic field on superconductivity, self-consistently within a BCS mean field model, for a clean 3D metal thin film. The electrostatic change in superconducting condensation energy scales as $\mu^{-1}$ close to subband edges as a function of the Fermi energy $\mu$, and follows 3D scaling $\mu^{-2}$ away from them. We discuss nonlinearities beyond gate effect, and contrast results to recent experiments.

---Josephson effectsuprajohtavuusFOS: Physical sciences02 engineering and technology01 natural sciencessuprajohteetSuperconductivity (cond-mat.supr-con)superconducting phase transitionElectric fieldCondensed Matter::Superconductivity0103 physical sciencesThin film010306 general physicsScalingCondensed Matter::Quantum GasesSuperconductivityPhysicsCondensed matter physicsCondensed Matter - SuperconductivityFermi energy021001 nanoscience & nanotechnologyMean field theorythin filmsmesoscopicsohutkalvot0210 nano-technologyEnergy (signal processing)Physical Review B
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Optical properties of GaSe, characterization and simulation

2021

Abstract The study focuses on structural and optical characterizations and properties of the GaSe lamellar material in one hand and on a numerical simulation of the photovoltaic properties of the ITO/GaSe heterojunction in a second hand. A few layers of GaSe were exfoliated from bulk GaSe on PET substrate. The optical transmission was recorded at room temperature. It shows that GaSe exhibits both indirect and direct band gaps of about 1.92 and 2.2 eV respectively. A value, as high as 104 cm−1, of the absorption coefficient was obtained. The corresponding refractive index has been determined numerically according to the Sellmeier and Cauchy models. The interesting value of absorption shows o…

010302 applied physicsCondensed Matter::Quantum GasesMaterials scienceComputer simulationbusiness.industryBand gapHeterojunction02 engineering and technologyÒptica021001 nanoscience & nanotechnology01 natural sciencesCharacterization (materials science)Attenuation coefficient0103 physical sciencesOptoelectronicsLamellar structure0210 nano-technologybusinessAbsorption (electromagnetic radiation)Refractive indexMaterials
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Two-qubit entanglement dynamics for two different non-Markovian environments

2009

We study the time behavior of entanglement between two noninteracting qubits each immersed in its own environment for two different non-Markovian conditions: a high-$Q$ cavity slightly off-resonant with the qubit transition frequency and a nonperfect photonic band-gap, respectively. We find that revivals and retardation of entanglement loss may occur by adjusting the cavity-qubit detuning, in the first case, while partial entanglement trapping occurs in non-ideal photonic-band gap.

03.67.Mn Entanglement measures witnesses and other characterizationCondensed Matter::Quantum GasesPhysicsQuantum Physicsbusiness.industryDynamics (mechanics)FOS: Physical sciencesMarkov process03.65.Ud Entanglement and quantum nonlocality (e.g. EPR paradox Bell's inequalities GHZ states etc.)Quantum PhysicsTrappingQuantum entanglementCondensed Matter PhysicsAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della Materiasymbols.namesake03.67.Mn Entanglement measures witnesses and other characterizations; 03.65.Ud Entanglement and quantum nonlocality (e.g. EPR paradox Bell's inequalities GHZ states etc.); 03.67.Lx Quantum computation architectures and implementationsQuantum mechanicsQubitsymbolsPhotonicsQuantum Physics (quant-ph)business03.67.Lx Quantum computation architectures and implementationsMathematical Physics
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Phase separations induced by a trapping potential in one-dimensional fermionic systems as a source of core-shell structures

2018

Ultracold fermionic gases in optical lattices give a great opportunity for creating different types of novel states. One of them is phase separation induced by a trapping potential between different types of superfluid phases. The core-shell structures, occurring in systems with a trapping potential, are a good example of such separations. The types and the sequences of phases which emerge in such structures can depend on spin-imbalance, shape of the trap and on-site interaction strength. In this work, we investigate the properties of such structures within an attractive Fermi gas loaded in the optical lattice, in the presence of the trapping potential and their relations to the phase diagr…

0301 basic medicineWork (thermodynamics)lcsh:MedicineFOS: Physical sciencesTrappingMolecular physicsArticleSuperconducting properties and materialsTrap (computing)Superfluidity03 medical and health sciences0302 clinical medicinePhase (matter)lcsh:ScienceUltracold gasesPhase diagramPhysicsCondensed Matter::Quantum GasesOptical latticeMultidisciplinarylcsh:R030104 developmental biologyQuantum Gases (cond-mat.quant-gas)lcsh:QCondensed Matter - Quantum GasesFermi gas030217 neurology & neurosurgery
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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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Trap-limited mobility in space-charge limited current in organic layers

2009

Space-charge limited current transport in organic devices, relevant to the operation of a range of organic optoelectronic devices, is analyzed in the frequency domain. The classical multiple trapping picture with one transport state and one trap level is used as the basis for the descriptions. By varying the energetic and kinetic properties of the traps, we show that the admittance and the capacitance spectra are considerably modified depending on the interplay between the trap-limited mobility and the trap kinetics. We point out that capacitance steps at low-frequency, usually found in experiments, are observed only for slow traps. © 2008 Elsevier B.V. All rights reserved.

AdmittanceCapacitanceTrappingCapacitanceBiomaterialsTrap (computing)OpticsMaterials ChemistryOLEDPhysics::Atomic PhysicsElectrical and Electronic EngineeringElectrical impedanceMobilityCondensed Matter::Quantum GasesOrganic electronicsChemistrybusiness.industryImpedanceGeneral ChemistryCondensed Matter PhysicsSpace chargeTrapElectronic Optical and Magnetic MaterialsOLEDChemical physicsTransport in organic materialsbusinessOrganic Electronics
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Polar bosons in one-dimensional disordered optical lattices

2013

We analyze the effects of disorder and quasi-disorder on the ground-state properties of ultra-cold polar bosons in optical lattices. We show that the interplay between disorder and inter-site interactions leads to rich phase diagrams. A uniform disorder leads to a Haldane-insulator phase with finite parity order, whereas the density-wave phase becomes a Bose-glass at very weak disorder. For quasi-disorder, the Haldane insulator connects with a gapped generalized incommesurate density wave without an intermediate critical region.

Anderson localization[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]PACS : 67.85.-d 05.30.Jp 61.44.Fw 75.10.PqFOS: Physical sciences01 natural sciencesCondensed Matter::Disordered Systems and Neural NetworksUltracold atoms010305 fluids & plasmasDensity wave theoryCondensed Matter - Strongly Correlated ElectronsUltracold atomQuantum mechanics0103 physical sciencesAnderson localization010306 general physicsBosonPhase diagramPhysicsCondensed Matter::Quantum Gasesdipolar interactionsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Parity (physics)Disordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksAubry-André transitionCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsQuantum Gases (cond-mat.quant-gas)PolarCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum Gases
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Ultracold Rare-Earth Magnetic Atoms with an Electric Dipole Moment

2018

We propose a new method to produce an electric and magnetic dipolar gas of ultracold dysprosium atoms. The pair of nearly degenerate energy levels of opposite parity, at 17513.33 cm$^{-1}$ with electronic angular momentum $J=10$, and at 17514.50 cm$^{-1}$ with $J=9$, can be mixed with an external electric field, thus inducing an electric dipole moment in the laboratory frame. For field amplitudes relevant to current-day experiments, we predict a magnetic dipole moment up to 13 Bohr magnetons, and an electric dipole moment up to 0.22 Debye, which is similar to the values obtained for alkali-metal diatomics. When a magnetic field is present, we show that the electric dipole moment is strongly…

Angular momentumAtomic Physics (physics.atom-ph)General Physics and AstronomyFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesAtomicPhysics - Atomic Physics010305 fluids & plasmas[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Electric field0103 physical sciencesPhysics::Atomic Physics010306 general physicsPhysicsQuantum PhysicsMagnetic moment[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Degenerate energy levelsMolecularand Optical Physics3. Good healthMagnetic fieldElectric dipole momentDipoleAmplitudeQuantum Gases (cond-mat.quant-gas)[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Atomic physicsCondensed Matter - Quantum GasesQuantum Physics (quant-ph)
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