Search results for "Hyperfine transition"

showing 2 items of 2 documents

Lifetimes and g-factors of the HFS states in H-like and Li-like bismuth

2018

The LIBELLE experiment performed at the experimental storage ring (ESR) at the GSI Helmholtz Center for Heavy Ion Research in Darmstadt, Germany, has successfully determined the ground state hyperfine (HFS) splittings in hydrogen-like ($^{209}\rm{Bi}^{82+}$) and lithium-like ($^{209}\rm{Bi}^{80+}$) bismuth. The study of HFS transitions in highly charged ions enables precision tests of QED in extreme electric and magnetic fields otherwise not attainable in laboratory experiments. Besides the transition wavelengths the time resolved detection of fluorescence photons following the excitation of the ions by a pulsed laser system also allows to extract lifetimes of the upper HFS levels and g-fac…

IONSGeneral PhysicsAtomic Physics (physics.atom-ph)0205 Optical PhysicsFOS: Physical scienceschemistry.chemical_elementg-factorsElectronPhysics Atomic Molecular & ChemicalHYPERFINE01 natural sciencesPhysics - Atomic PhysicsIonBismuth0103 physical sciences0307 Theoretical and Computational ChemistryPhysics::Atomic Physicshyperfine transitions010306 general physicsHyperfine structurePrecision tests of QEDPhysicsScience & Technology010308 nuclear & particles physicsPhysicsOpticsCondensed Matter PhysicsAtomic and Molecular Physics and OpticsMagnetic fieldchemistryPhysical Sciences0202 Atomic Molecular Nuclear Particle and Plasma PhysicslifetimesAtomic physicsGround statehighly charged ionsExcitationJournal of Physics B: Atomic, Molecular and Optical Physics
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Saturated absorption spectroscopy: elimination of crossover resonances by use of a nanocell

2007

It is demonstrated that velocity selective optical pumping/saturation resonances of reduced absorption in a Rb vapor nanocell with thickness \textit{L=} $\lambda $, 2$\lambda $, and 3$\lambda $ (resonant wavelength $\lambda $ = 780 nm) allow the complete elimination of crossover (CO) resonances. We observe well pronounced resonances corresponding to the F$_{g}=3$ $\to $ F$_{e}=2,3,4$ hyperfine transitions of the $^{85}$Rb D$_{2}$ line with linewidths close to the natural width. A small CO resonance located midway between F$_{g}=3$ $\to $ F$_{e}=3$ and F$_{g}=3$ $\to$ F$_{e}=4$ transitions appears only for \textit{L} = 4$\lambda $. The D$_{2}$ line ($\lambda $ = 852 nm) in a Cs nanocell exhi…

StandardsOptical pumping[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Saturated absorption spectroscopyFOS: Physical sciencesPhysics - Classical PhysicsLambda01 natural sciencesIndustrial and Manufacturing Engineering010309 opticssymbols.namesakeAbsorption spectroscopy[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciencesFrequency measurementLine widthsRubidium 85Physics::Atomic Physics010306 general physicsInstrumentationHyperfine structure[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]PhysicsZeeman effectResonanceClassical Physics (physics.class-ph)Zeeman effectNanocellCondensed Matter PhysicsAtomic and Molecular Physics and Optics3. Good healthMagnetic fieldWavelengthHyperfine transitionsymbolsRubidium AtomsMagnetic field effectsAtomic physicsOptical saturation
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