Search results for "quantum physics"

showing 10 items of 1595 documents

Quantum localization and bound state formation in Bose-Einstein condensates

2010

We discuss the possibility of exponential quantum localization in systems of ultracold bosonic atoms with repulsive interactions in open optical lattices without disorder. We show that exponential localization occurs in the maximally excited state of the lowest energy band. We establish the conditions under which the presence of the upper energy bands can be neglected, determine the successive stages and the quantum phase boundaries at which localization occurs, and discuss schemes to detect it experimentally by visibility measurements. The discussed mechanism is a particular type of quantum localization that is intuitively understood in terms of the interplay between nonlinearity and a bou…

Atomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesSpectral linelocalization010305 fluids & plasmaslaw.inventionPhysics - Atomic PhysicslawQuantum mechanics0103 physical sciencesBound state010306 general physicsElectronic band structureQuantumPhysicsQuantum PhysicsAtomic and Molecular Physics and Optics3. Good healthExponential functionWeak localizationQuantum Gases (cond-mat.quant-gas)Excited stateQuantum electrodynamicsQuantum Physics (quant-ph)Condensed Matter - Quantum GasesBose–Einstein condensate
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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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Experimental benchmarking of quantum control in zero-field nuclear magnetic resonance

2017

Zero-field nuclear magnetic resonance (NMR) provides complementary analysis modalities to those of high-field NMR and allows for ultra-high-resolution spectroscopy and measurement of untruncated spin-spin interactions. Unlike for the high-field case, however, universal quantum control -- the ability to perform arbitrary unitary operations -- has not been experimentally demonstrated in zero-field NMR. This is because the Larmor frequency for all spins is identically zero at zero field, making it challenging to individually address different spin species. We realize a composite-pulse technique for arbitrary independent rotations of $^1$H and $^{13}$C spins in a two-spin system. Quantum-inform…

Atomic Physics (physics.atom-ph)FOS: Physical sciencesQuantum simulator02 engineering and technology01 natural sciencesPhysics - Atomic PhysicsNuclear magnetic resonanceControlled NOT gatePhysics - Chemical Physics0103 physical sciencesQuantum metrology010306 general physicsSpin (physics)Chemical Physics (physics.chem-ph)Larmor precessionPhysicsQuantum PhysicsMultidisciplinarySpins500Nuclear magnetic resonance spectroscopy021001 nanoscience & nanotechnologyCondensed Matter::Strongly Correlated Electronsddc:500Quantum Physics (quant-ph)0210 nano-technologyRealization (systems)
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Measurement of untruncated nuclear spin interactions via zero- to ultralow-field nuclear magnetic resonance

2015

Zero- to ultra-low-field nuclear magnetic resonance (ZULF NMR) provides a new regime for the measurement of nuclear spin-spin interactions free from effects of large magnetic fields, such as truncation of terms that do not commute with the Zeeman Hamiltonian. One such interaction, the magnetic dipole-dipole coupling, is a valuable source of spatial information in NMR, though many terms are unobservable in high-field NMR, and the coupling averages to zero under isotropic molecular tumbling. Under partial alignment, this information is retained in the form of so-called residual dipolar couplings. We report zero- to ultra-low-field NMR measurements of residual dipolar couplings in acetonitrile…

Atomic Physics (physics.atom-ph)Fluids & Plasmasphysics.chem-phFOS: Physical sciences010402 general chemistryJ-couplingphysics.atom-ph01 natural sciencesPhysics - Atomic Physicssymbols.namesakeEngineeringNuclear magnetic resonancequant-phPhysics - Chemical Physics0103 physical sciencesMagnetization transfer010306 general physicsChemical Physics (physics.chem-ph)PhysicsQuantum PhysicsZeeman effectCondensed matter physicsCondensed Matter Physics0104 chemical sciences3. Good healthElectronic Optical and Magnetic MaterialsMagnetic fieldSolid-state nuclear magnetic resonanceResidual dipolar couplingPhysical SciencesChemical SciencessymbolsQuantum Physics (quant-ph)Two-dimensional nuclear magnetic resonance spectroscopyMagnetic dipole–dipole interaction
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Compact two-electron wave function for bond dissociation and Van der Waals interactions: A natural amplitude assessment

2014

Electron correlations in molecules can be divided in short range dynamical correlations, long range Van der Waals type interactions and near degeneracy static correlations. In this work we analyze for a one-dimensional model of a two-electron system how these three types of correlations can be incorporated in a simple wave function of restricted functional form consisting of an orbital product multiplied by a single correlation function $f(r_{12})$ depending on the interelectronic distance $r_{12}$. Since the three types of correlations mentioned lead to different signatures in terms of the natural orbital (NO) amplitudes in two-electron systems we make an analysis of the wave function in t…

Atomic Physics (physics.atom-ph)General Physics and AstronomyFOS: Physical sciencesPhysics - Atomic Physicssymbols.namesakeCondensed Matter - Strongly Correlated ElectronsAtomic orbitalQuantum mechanicsPhysics - Chemical PhysicsPhysics::Atomic PhysicsSDG 7 - Affordable and Clean EnergyPhysical and Theoretical ChemistryWave functionAnsatzPhysicsChemical Physics (physics.chem-ph)Quantum Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyta114Electronic correlationStrongly Correlated Electrons (cond-mat.str-el)Computational Physics (physics.comp-ph)Diatomic molecule3. Good healthBond lengthAmplitudesymbolsvan der Waals forceQuantum Physics (quant-ph)Physics - Computational Physics
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Long-range interactions and the sign of natural amplitudes in two-electron systems

2013

In singlet two-electron systems the natural occupation numbers of the one-particle reduced density matrix are given as squares of the natural amplitudes which are defined as the expansion coefficients of the two-electron wave function in a natural orbital basis. In this work we relate the sign of the natural amplitudes to the nature of the two-body interaction. We show that long-range Coulomb-type interactions are responsible for the appearance of positive amplitudes and give both analytical and numerical examples that illustrate how the long-distance structure of the wave function affects these amplitudes. We further demonstrate that the amplitudes show an avoided crossing behavior as func…

Atomic Physics (physics.atom-ph)General Physics and AstronomyInteraction strengthFOS: Physical sciences02 engineering and technologyElectron01 natural sciencesPhysics - Atomic PhysicsCondensed Matter - Strongly Correlated Electronssymbols.namesakeQuantum mechanics0103 physical sciencesCoulombPhysical and Theoretical ChemistryWave functionPhysicsQuantum Physicsta114010304 chemical physicsStrongly Correlated Electrons (cond-mat.str-el)Avoided crossingComputational Physics (physics.comp-ph)021001 nanoscience & nanotechnologyAmplitudesymbolsReduced density matrix0210 nano-technologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Physics - Computational Physics
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Optical Shielding of Destructive Chemical Reactions between Ultracold Ground-State NaRb Molecules

2020

Polar quantum gases represent promising platforms for studying many-body physics and strongly correlated systems with possible applications e.g. in quantum simulation or quantum computation. Due to their large permanent electric dipole moment polar molecules in electric field exhibit strong long-range anisotropic dipole-dipole interactions (DDIs). The creation and trapping of ultracold dipolar diatomic molecules of various species are feasible in many experimental groups nowadays. However long time trapping is still a challenge even in the case of the so called nonreactive molecules which are supposed to be immune against inelastic collisions in their absolute ground state [1] . Various hyp…

Atomic Physics (physics.atom-ph)Inelastic collisionGeneral Physics and AstronomyFOS: Physical sciencesQuantum simulator01 natural sciences7. Clean energyMolecular physicslaw.inventionPhysics - Atomic Physics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]law0103 physical sciencesMoleculeSpontaneous emissionPhysics::Atomic Physics010306 general physicsComputingMilieux_MISCELLANEOUSPhysics[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Rotational–vibrational spectroscopyLaserDiatomic moleculeDipoleElectric dipole momentQuantum Gases (cond-mat.quant-gas)Excited stateAtom optics[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Atomic physicsCondensed Matter - Quantum GasesGround state
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Sawtooth-wave adiabatic-passage slowing of dysprosium

2018

We report on sawtooth wave adiabatic passage (SWAP) slowing of bosonic and fermionic dysprosium isotopes by using a 136 kHz wide transition at 626 nm. A beam of precooled atoms is further decelerated in one dimension by the SWAP force and the amount of atoms at near zero velocity is measured. We demonstrate that the SWAP slowing can be twice as fast as in a conventional optical molasses operated on the same transition. In addition, we investigate the parameter range for which the SWAP force is efficiently usable in our set-up, and relate the results to the adiabaticity condition. Furthermore, we add losses to the hyperfine ground-state population of fermionic dysprosium during deceleration …

Atomic Physics (physics.atom-ph)PopulationFOS: Physical scienceschemistry.chemical_elementSawtooth wave01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmas0103 physical sciencesPhysics::Atomic Physics010306 general physicsAdiabatic processeducationHyperfine structurePhysicsQuantum PhysicsRange (particle radiation)education.field_of_studychemistryQuantum Gases (cond-mat.quant-gas)Optical molassesDysprosiumAtomic physicsQuantum Physics (quant-ph)Condensed Matter - Quantum GasesBeam (structure)Physical Review A
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Observation of a narrow inner-shell orbital transition in atomic erbium at 1299 nm

2021

We report on the observation and coherent excitation of atoms on the narrow inner-shell orbital transition, connecting the erbium ground state $[\mathrm{Xe}] 4f^{12} (^3\text{H}_6)6s^{2}$ to the excited state $[\mathrm{Xe}] 4f^{11}(^4\text{I}_{15/2})^05d (^5\text{D}_{3/2}) 6s^{2} (15/2,3/2)^0_7$. This transition corresponds to a wavelength of 1299 nm and is optically closed. We perform high-resolution spectroscopy to extract the $g_J$-factor of the $1299$-nm state and to determine the frequency shift for four bosonic isotopes. We further demonstrate coherent control of the atomic state and extract a lifetime of 178(19) ms which corresponds to a linewidth of 0.9(1) Hz. The experimental findi…

Atomic Physics (physics.atom-ph)chemistry.chemical_elementFOS: Physical sciences01 natural sciences010305 fluids & plasmasPhysics - Atomic PhysicsErbium[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Polarizability0103 physical sciences010306 general physicsSpectroscopyPhysicsQuantum Physics[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]3. Good healthWavelengthchemistryCoherent controlQuantum Gases (cond-mat.quant-gas)Excited state[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Atomic physicsGround stateQuantum Physics (quant-ph)Condensed Matter - Quantum GasesExcitation
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Anisotropic light-shift and magic-polarization of the intercombination line of Dysprosium atoms in a far-detuned dipole trap

2018

We characterize the anisotropic differential ac-Stark shift for the Dy $626$ nm intercombination transition, induced in a far-detuned $1070$ nm optical dipole trap, and observe the existence of a "magic polarization" for which the polarizabilities of the ground and excited states are equal. From our measurements we extract both the scalar and tensorial components of the dynamic dipole polarizability for the excited state, $\alpha_E^\text{s} = 188 (12)\,\alpha_\text{0}$ and $\alpha_E^\text{t} = 34 (12)\,\alpha_\text{0}$, respectively, where $\alpha_\text{0}$ is the atomic unit for the electric polarizability. We also provide a theoretical model allowing us to predict the excited state polari…

Atomic Physics (physics.atom-ph)chemistry.chemical_elementFOS: Physical sciences01 natural sciencesAtomic units010305 fluids & plasmasPhysics - Atomic Physics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Polarizability0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsAnisotropyDoppler coolingPhysicsCondensed Matter::Quantum GasesQuantum Physics[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Polarization (waves)3. Good healthDipolechemistryQuantum Gases (cond-mat.quant-gas)Excited stateDysprosium[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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