Publication | Open Access
Vacuum-ultraviolet spectroscopy of Xe: Hyperfine splittings, isotope shifts, and isotope-dependent ionization energies
72
Citations
11
References
2001
Year
Isotope-dependent Ionization EnergiesX-ray SpectroscopyNuclear PhysicsEngineeringMagnetic ResonanceElectronic Excited StateSpectroscopic PropertySpectra-structure CorrelationX-ray FluorescenceVacuum-ultraviolet SpectroscopyIon EmissionIonization EnergyOther IsotopesPhysicsAtomic PhysicsPhysical ChemistryQuantum ChemistryHyperfine SplittingsNatural SciencesSpectroscopyHigh-resolution Spectroscopy
High-resolution spectroscopy of xenon is performed on four transitions from the ${5p}^{6}{}^{1}{S}_{0}$ ground state to the ${5d}^{\ensuremath{'}}[3/2{]}_{1},$ $8d[1/2{]}_{1},$ $8d[3/2{]}_{1},$ and ${7s}^{\ensuremath{'}}[1/2{]}_{1}$ excited states $(jl$-coupling notation) by means of $1\mathrm{VUV}+1\mathrm{UV}$ photoionization spectroscopy. Spectra of all nine stable isotopes are resolved enabling the determination of the hyperfine splittings and isotope shifts. Magnetic dipole (for both ${}^{129}\mathrm{Xe}$ and ${}^{131}\mathrm{Xe})$ and electric quadrupole (for ${}^{131}\mathrm{Xe})$ hyperfine splitting constants are derived for all four excited states. Mass and field shift contributions to the isotope shifts are separated using King plots relative to existing accurate isotope shift values. A high field shift factor, even for the transitions in which no s electron is involved, is deduced. From precise calibration of the transition frequencies an accurate value for the ionization energy of ${}^{136}\mathrm{Xe},$ ${E}_{3/2}^{136}=97833.805(11) {\mathrm{cm}}^{\ensuremath{-}1},$ is derived. In addition, values of the ionization energies for all other isotopes are determined.
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