Search results for "physics.atom-ph"

showing 10 items of 395 documents

Evidence for degenerate mirrorless lasing in alkali metal vapor: forward beam magneto-optical experiment

2018

We report an experimental observation of degenerate mirrorless lasing in forward direction under excitation of a dilute atomic Rb vapor with a single linearly polarized cw laser light resonant with cycling Fe > Fg atomic D2 transitions. Light polarized orthogonally to the laser light is generated for the input light intensity exceeding a threshold value of about 3 mW/cm^2. Application of a transverse magnetic field directed along the input light polarization reveals a sharp about 20 mG wide magnetic resonance centered at B = 0. Increasing the incident light intensity from 3 to 300 mW/cm^2, the generated light undergoes rapid amplitude increase followed by a decline and resonance broadeni…

PhysicsAtomic Physics (physics.atom-ph)Linear polarizationFOS: Physical sciencesResonanceCondensed Matter PhysicsPopulation inversionLaserPolarization (waves)01 natural sciencesRayAtomic and Molecular Physics and OpticsPhysics - Atomic Physicslaw.invention010309 opticsLight intensitylaw0103 physical sciencesAtomic physics010306 general physicsLasing thresholdJournal of Physics B: Atomic, Molecular and Optical Physics
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Revisiting spin-dependent forces mediated by new bosons : potentials in the coordinate-space representation for macroscopic- and atomic-scale experim…

2019

The exchange of spin-0 or spin-1 bosons between fermions or spin-polarised macroscopic objects gives rise to various spin-dependent potentials. We derive the coordinate-space non-relativistic potentials induced by the exchange of such bosons, including contact terms that can play an important role in atomic-scale phenomena, and correct for errors and omissions in the literature. We summarise the properties of the potentials and their relevance for various types of experiments. These potentials underpin the interpretation of experiments that search for new bosons, including spectroscopy, torsion-pendulum measurements, magnetometry, parity nonconservation and electric dipole moment experiment…

PhysicsAtomic Physics (physics.atom-ph)Physics beyond the Standard ModelFOS: Physical sciencesParity (physics)Fermion01 natural sciencesAtomic units3. Good health010305 fluids & plasmasPhysics - Atomic PhysicsElectric dipole momentTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCP violationCoordinate space010306 general physicsBoson
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Using optical clock transitions in Cu II and Yb III for time-keeping and search for new physics

2021

We study the $^1$S$_0 - ^3$D$_2$ and $^1$S$_0 - ^3$D$_3$ transitions in Cu II and the $^1$S$_0 - ^3$P$^{\rm o}_2$ transition in Yb III as possible candidates for the optical clock transitions. A recently developed version of the configuration (CI) method, designed for a large number of electrons above closed-shell core, is used to carry out the calculation. We calculate excitation energies, transition rates, lifetimes, scalar static polarizabilities of the ground and clock states, and blackbody radiation shift. We demonstrate that the considered transitions have all features of the clock transition leading to prospects of highly accurate measurements. Search for new physics, such as time va…

PhysicsAtomic Physics (physics.atom-ph)Physics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesElectronConfiguration interaction01 natural sciences7. Clean energy010305 fluids & plasmasPhysics - Atomic Physics0103 physical sciencesClock transitionOptical clockBlack-body radiationAtomic physics010306 general physicsExcitation
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Nobelium energy levels and hyperfine structure constants

2018

Advances in laser spectroscopy of superheavy ($Z>100$) elements enabled determination of the nuclear moments of the heaviest nuclei, which requires high-precision atomic calculations of the relevant hyperfine structure (HFS) constants. Here, we calculated the HFS constants and energy levels for a number of nobelium (Z=102) states using the hybrid approach, combining linearized coupled-cluster and configuration interaction methods. We also carried out an extensive study of the No energies using 16-electron configuration interaction method to determine the position of the (5f^{13}7s^2 6d) and (5f^{13}7s^2 7p) levels with a hole in the 5f shell to evaluate their potential effect on the hype…

PhysicsAtomic Physics (physics.atom-ph)Potential effectchemistry.chemical_elementFOS: Physical sciencesConfiguration interactionHybrid approach01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmaschemistry0103 physical sciencesNobeliumAtomic physics010306 general physicsSpectroscopyHyperfine structureEnergy (signal processing)
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Initial state dependence of a quantum-resonance ratchet

2016

We demonstrate quantum resonance ratchets created with Bose-Einstein condensates exposed to pulses of an off-resonant standing light wave. We show how some of the basic properties of the ratchets are controllable through the creation of different initial states of the system. In particular, our results prove that through an appropriate choice of initial state it is possible to reduce the extent to which the ratchet state changes with respect to time. We develop a simple theory to explain our results and indicate how ratchets might be used as part of a matter wave interferometer or quantum-random walk experiment.

PhysicsAtomic Physics (physics.atom-ph)RatchetLight waveFOS: Physical sciencesQuantum resonance01 natural sciences010305 fluids & plasmasPhysics - Atomic PhysicsInterferometryQuantum mechanics0103 physical sciencesState dependenceQuantum walk010306 general physics
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Alignment-to-orientation conversion in a magnetic field at nonlinear excitation of theD2line of rubidium: Experiment and theory

2015

We studied alignment-to-orientation conversion caused by excited-state level crossings in a nonzero magnetic field of both atomic rubidium isotopes. Experimental measurements were performed on the transitions of the $D_2$ line of rubidium. These measured signals were described by a theoretical model that takes into account all neighboring hyperfine transitions, the mixing of magnetic sublevels in an external magnetic field, the coherence properties of the exciting laser radiation, and the Doppler effect. In the experiments laser induced fluorescence (LIF) components were observed at linearly polarized excitation and their difference was taken afterwards. By observing the two oppositely circ…

PhysicsAtomic Physics (physics.atom-ph)business.industryLinear polarizationFOS: Physical scienceschemistry.chemical_elementLaserAtomic and Molecular Physics and OpticsIsotopes of rubidiumPhysics - Atomic Physicslaw.inventionRubidiumMagnetic fieldOpticschemistrylawPhysics::Atomic PhysicsAtomic physicsbusinessHyperfine structureExcitationCoherence (physics)Physical Review A
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Laser spectroscopy of the 1001nm ground state transition in dysprosium

2018

We present a direct excitation of the presumably ultranarrow $1001\ensuremath{-}\mathrm{nm}$ ground-state transition in atomic dysprosium. By using resonance ionization spectroscopy with pulsed Ti:sapphire lasers at a hot cavity laser ion source, we were able to measure the isotopic shifts in the $1001\ensuremath{-}\mathrm{nm}$ line between all seven stable isotopes. Furthermore, we determined the upper level energy from the atomic transition frequency of the $^{164}\mathrm{Dy}$ isotope as $9991.004(1)\phantom{\rule{0.16em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}1}$ and confirm the level energy listed in the NIST database. Since a sufficiently narrow natural linewidth is an essential prerequisit…

PhysicsAtomic Physics (physics.atom-ph)chemistry.chemical_elementFOS: Physical sciencesLaser01 natural sciencesIon source010305 fluids & plasmas3. Good healthlaw.inventionPhysics - Atomic PhysicsLaser linewidthchemistrylawExcited state0103 physical sciencesDysprosiumPhysics::Atomic PhysicsAtomic physics010306 general physicsSpectroscopyGround stateEnergy (signal processing)
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Molecular parity nonconservation in nuclear spin couplings

2017

The weak interaction does not conserve parity, which is apparent in many nuclear and atomic phenomena. However, thus far, parity nonconservation has not been observed in molecules. Here we consider nuclear-spin-dependent parity nonconserving contributions to the molecular Hamiltonian. These contributions give rise to a parity nonconserving indirect nuclear spin-spin coupling which can be distinguished from parity conserving interactions in molecules of appropriate symmetry, including diatomic molecules. We estimate the magnitude of the coupling, taking into account relativistic corrections. Finally, we propose and simulate an experiment to detect the parity nonconserving coupling using liqu…

PhysicsChemical Physics (physics.chem-ph)Antisymmetric relationAtomic Physics (physics.atom-ph)FOS: Physical sciencesParity (physics)010402 general chemistry01 natural sciences5300104 chemical sciencesPhysics - Atomic PhysicsQuantum mechanicsPhysics - Chemical Physics0103 physical sciencesddc:530Physics::Atomic Physics010306 general physics
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The potential of the ground state of NaRb

2004

The X$^{1}\Sigma ^{+}$ state of NaRb was studied by Fourier transform spectroscopy. An accurate potential energy curve was derived from more than 8800 transitions in isotopomers $^{23}$Na$^{85}$Rb and $^{23}$Na$^{87}$Rb. This potential reproduces the experimental observations within their uncertainties of 0.003 \rcm to 0.007 \rcm. The outer classical turning point of the last observed energy level ($v''=76$, $J''=27$) lies at $\approx 12.4$ \AA, leading to a energy of 4.5 \rcm below the ground state asymptote.

PhysicsChemical Physics (physics.chem-ph)Atomic Physics (physics.atom-ph)Physics - Chemical PhysicsFOS: Physical sciencesTurning pointAtomic physicsGround stateAtomic and Molecular Physics and OpticsEnergy (signal processing)Physics - Atomic Physics
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Collisional and thermal ionization of sodium Rydberg atoms I. Experiment for nS and nD atoms with n=8-20

2005

Collisional and thermal ionization of sodium nS and nD Rydberg atoms with n=8-20 has been studied. The experiments were performed using a two-step pulsed laser excitation in an effusive atomic beam at atom density of about 2 10^{10} cm^{-3}. Molecular and atomic ions from associative, Penning, and thermal ionization processes were detected. It has been found that the atomic ions were created mainly due to photoionization of Rydberg atoms by photons of blackbody radiation at the ambient temperature of 300K. Blackbody ionization rates and effective lifetimes of Rydberg states of interest were determined. The molecular ions were found to be from associative ionization in Na(nL)+Na(3S) collisio…

PhysicsChemical Physics (physics.chem-ph)Atomic Physics (physics.atom-ph)Thermal ionizationFOS: Physical sciencesPhotoionizationCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIonPhysics - Atomic Physicssymbols.namesakeIonizationPhysics - Chemical PhysicsRydberg atomAtomRydberg formulasymbolsPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physicsExcitation
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