Core effects on the polarization of optical Rydberg transitions following 
electron capture into slow, highly ionized neon recoil ions

Lembo, L. J.; Danzmann, Karsten; Stoller, Ch.; Meyerhof, W. E.; Hansch, T. W.

doi:10.1103/PhysRevA.37.1141

Item

ITEM ACTIONSEXPORT

Add to Basket

Release HistoryDetailsSummary

Released

Journal Article

Core effects on the polarization of optical Rydberg transitions following electron capture into slow, highly ionized neon recoil ions

MPS-Authors

/persons/resource/persons40437

Danzmann, Karsten
Laser Interferometry & Gravitational Wave Astronomy, AEI-Hannover, MPI for Gravitational Physics, Max Planck Society;

External Resource

No external resources are shared

Fulltext (restricted access)

There are currently no full texts shared for your IP range.

Fulltext (public)

372201.pdf
(Publisher version), 3MB

Supplementary Material (public)

There is no public supplementary material available

Citation

Lembo, L. J., Danzmann, K., Stoller, C., Meyerhof, W. E., & Hansch, T. W. (1988). Core effects on the polarization of optical Rydberg transitions following electron capture into slow, highly ionized neon recoil ions. Physical Review A, 37(4), 1141-1151. doi:10.1103/PhysRevA.37.1141.

Cite as: https://hdl.handle.net/11858/00-001M-0000-0013-5D6D-0

Abstract

Polarization measurements have been performed and emission spectra in the visible and near ultraviolet have been acquired for transitions between Rydberg states of slow, highly charged neon ions (Neq+, with q=10–5, and v≊0.09 a.u.), following electron capture from Na. Resolvable line splittings appear in those spectra for which the incoming projectile ions carry L-shell core electrons. The optical emission cross sections are much smaller for these ions and the radiation is significantly depolarized relative to those ions whose transitions are seen as structureless. These effects are attributed to the inhibition of Stark mixing by core interactions.