Search results for "formula"

showing 10 items of 755 documents

Rydberg excitation of trapped cold ions: a detailed case study

2011

We provide a detailed theoretical and conceptual study of a planned experiment to excite Rydberg states of ions trapped in a Paul trap. The ultimate goal is to exploit the strong state dependent interactions between Rydberg ions to implement quantum information processing protocols and to simulate the dynamics of strongly interacting spin systems. We highlight the promises of this approach when combining the high degree of control and readout of quantum states in trapped ion crystals with the novel and fast gate schemes based on interacting giant Rydberg atomic dipole moments. We discuss anticipated theoretical and experimental challenges on the way towards its realization.

PhysicsQuantum PhysicsAtomic Physics (physics.atom-ph)FOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmasIonsymbols.namesakeDipoleQuantum state0103 physical sciencesRydberg formulasymbolsPhysics::Atomic PhysicsIon trapAtomic physicsQuantum Physics (quant-ph)010306 general physicsSpin (physics)Realization (systems)ExcitationNew Journal of Physics
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Line shapes and time dynamics of the F��rster resonances between two Rydberg atoms in a time-varying electric field

2016

The observation of the Stark-tuned F\"orster resonances between Rydberg atoms excited by narrowband cw laser radiation requires usage of a Stark-switching technique in order to excite the atoms first in a fixed electric field and then to induce the interactions in a varied electric field, which is scanned across the F\"orster resonance. In our experiments with a few cold Rb Rydberg atoms we have found that the transients at the edges of the electric pulses strongly affect the line shapes of the F\"orster resonances, since the population transfer at the resonances occurs on a time scale of $\sim$100 ns, which is comparable with the duration of the transients. For example, a short-term ringin…

PhysicsQuantum PhysicsAtomic Physics (physics.atom-ph)FOS: Physical sciencesLaser01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmaslaw.inventionsymbols.namesakelawQuantum Gases (cond-mat.quant-gas)Time dynamicsElectric field0103 physical sciencesRydberg atomRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physicsCondensed Matter - Quantum Gases010306 general physicsQuantum Physics (quant-ph)ExcitationLine (formation)
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Spectroscopy of an ultracold Rydberg gas and signatures of Rydberg–Rydberg interactions

2005

We report on experiments on Rydberg–Rydberg interaction-induced effects in a gas of 87Rb Rydberg atoms. A compact setup for two-photon continuous-wave excitation of high-lying Rydberg states out of an ultracold atomic gas is presented. The performance of the apparatus is characterized by high-resolution spectroscopy of Rydberg states. Signatures of interaction-induced effects are identified by qualitatively analysing the dependence of Rydberg excitation spectra on the intensity and the duration of the second-step laser excitation.

PhysicsQuantum PhysicsCondensed Matter PhysicsLaserAtomic and Molecular Physics and Opticslaw.inventionsymbols.namesakelawUltracold atomExcited stateRydberg atomsymbolsRydberg formulaRydberg matterPhysics::Atomic PhysicsAtomic physicsSpectroscopyExcitationJournal of Physics B: Atomic, Molecular and Optical Physics
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Determination of quantum defect for the Rydberg P series of Ca II

2019

We present an experimental investigation of the Rydberg 23 P$_{1/2}$ state of laser-cooled $^{40}$Ca$^+$ ions in a radiofrequency ion trap. Using micromotion sideband spectroscopy on a narrow quadrupole transition, the oscillating electric field at the ion position was precisely characterised, and the modulation of the Rydberg transition due to this field was minimised. From a correlated fit to this P line and previously measured P and F level energies of Ca II, we have determined the ionization energy of 95 751.916(32) $\rm {cm}^{-1}$, in agreement with the accepted value, and the quantum defect for the $n$ P$_{1/2}$ states.

PhysicsQuantum PhysicsField (physics)Atomic Physics (physics.atom-ph)FOS: Physical sciencesCondensed Matter Physics01 natural sciencesAtomic and Molecular Physics and OpticsPhysics - Atomic PhysicsIon010309 opticssymbols.namesakeQuantum defect0103 physical sciencesQuadrupoleRydberg formulasymbolsIon trapPhysics::Atomic PhysicsAtomic physicsIonization energy010306 general physicsSpectroscopyQuantum Physics (quant-ph)
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QCD running in neutrinoless double beta decay: Short-range mechanisms

2016

16 pages.- 3 figures.- 2 tables

PhysicsQuantum chromodynamicsParticle physicsNuclear TheorySuperformula010308 nuclear & particles physicsPhysics beyond the Standard ModelFOS: Physical sciencesFermionRenormalization group01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Operator (computer programming)High Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)Double beta decay0103 physical sciencesEffective field theoryNuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
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Erratum to: Classical and Quantum Dynamics: From Classical Paths to Path Integrals

2017

PhysicsQuantum dynamicsQuantum mechanicsPath integral formulationQuantum chaosClassical limit
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Propagators for Particles in an External Magnetic Field

2001

In order to describe the propagation of a scalar particle in an external potential, we begin again with the path integral $$ K(r',t';r,0) = \int_{r,(0)}^{r',(t')} {[dr(t)]} \exp \left\{ {\frac{{\text{i}}} {\hbar }S[r(t)]} \right\} $$ (1) with $$ S[r(t)] = \int_0^{t'} {dt} L(r,\dot r). $$

PhysicsQuantum electrodynamicsPath integral formulationPropagatorOrder (ring theory)Scalar bosonWave functionMathematical physicsMagnetic field
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Spontaneous emission rates and energy shifts of a Rydberg rubidium atom close to an optical nanofiber

2020

The influence of an optical nanofiber on the spontaneous emission rates and Lamb shifts of a Rydberg rubidium atom in its close vicinity is investigated, in view of the implementation of a Rydberg-blockade-based quantum network.

PhysicsQuantum networkPhysics::OpticsQuantum PhysicsQuantum memorysymbols.namesakeNanofiberPhysics::Atomic and Molecular ClustersRydberg formulasymbolsSpontaneous emissionPhysics::Atomic PhysicsRubidium atomAtomic physicsEnergy (signal processing)OSA Quantum 2.0 Conference
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Effective Lagrangian approach to neutrinoless double beta decay and neutrino masses

2012

Neutrinoless double beta ($0\nu\beta\beta$) decay can in general produce electrons of either chirality, in contrast with the minimal Standard Model (SM) extension with only the addition of the Weinberg operator, which predicts two left-handed electrons in the final state. We classify the lepton number violating (LNV) effective operators with two leptons of either chirality but no quarks, ordered according to the magnitude of their contribution to \znbb decay. We point out that, for each of the three chirality assignments, $e_Le_L, e_Le_R$ and $e_Re_R$, there is only one LNV operator of the corresponding type to lowest order, and these have dimensions 5, 7 and 9, respectively. Neutrino masse…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Lepton numberPartícules (Física nuclear)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decayBeyond Standard ModelNeutrino PhysicsHigh Energy Physics::ExperimentNeutrinoLepton
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The CP-Conserving Direction

1998

A symmetry transformation is well defined in the case of an invariant theory, being the corresponding operator undetermined otherwise. However, we show that, even with CP violation, it is possible to determine the CP transformation by separating the Lagrangian of the Standard Model in a CP-conserving and a CP-violating part, in a unique way, making use of the empirically known quark mixing hierarchy. To order \lambda^3 for the Bd-system, the CP-conserving direction matches one of the sides of the (bd) unitarity triangle. We use this determination to calculate the rephasing invariant parameter \epsilon, which measures CP-mixing in the B0-B0bar system.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsUnitarityOperator (physics)High Energy Physics::PhenomenologyFísicaFOS: Physical sciencesInvariant theoryHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)CP violationInvariant (mathematics)Mixing (physics)Mathematical physics
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