Physical Review A · 1996 · 31 citations · 10 references
Natural SciencesPhysicsNuclear PhysicsQuantum MechanicsSpectroscopyAtomic SpectroscopyElectronic SpectroscopyFine StructureMicrowave SpectroscopyPrecision SpectroscopyRydberg AtomsAtomic Fine StructureDipole Moment DeterminationFine Structure Of Rydberg StatesGround State PropertiesMicrowave Spectroscopy Of Rydberg StatesNuclear Electric Quadrupole MomentQuadrupole InteractionRydberg Spectroscopy
Sixteen fine-structure intervals separating n=10 neon Rydberg levels with L=5, 6, 7, and 8 were measured with the precision of about \ifmmode\pm\else\textpm\fi{}00.2 MHz, using fast beam microwave-optical techniques. The measured fine-structure pattern is in good agreement with the predictions of an effective potential model, and this comparison leads to precise determinations of the quadrupole moment and dipole polarizabilities of the $^{2}$${\mathit{P}}_{3/2}$ ground state of the ${\mathrm{Ne}}^{+}$ ion: Q=-0.204 03(5)${\mathrm{ea}}_{0}^{2}$, ${\mathrm{\ensuremath{\alpha}}}_{\mathit{s}}$=1.3028(13)${\mathit{a}}_{0}^{3}$, ${\mathrm{\ensuremath{\alpha}}}_{\mathit{T}}$=-0.026(5)${\mathit{a}}_{0}^{3}$. The contributions of magnetic interactions to the Rydberg fine structure lead to a determination of the ${\mathrm{Ne}}^{+}$ ion's g value, ${\mathit{g}}_{\mathit{J}}$=1.354(21). All of these core parameters provide challenging tests of atomic structure calculations. The measurements also set a limit on the possible contributions to the fine structure due to a predicted geometric phase effect that is about an order of magnitude smaller than expected. \textcopyright{} 1996 The American Physical Society.
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