Monthly Archives: August 2013

Magic Rydberg

 

Rydberg electron in circular orbit can be attracted to laser intensity maxima. Thereby a laser beam can serve as a tractor beam for cold Rydberg atoms.

Rydberg atoms in circular states can be attracted to laser intensity maxima. Thereby a laser beam can serve as a tractor beam for cold Rydberg atoms.

Here is our recent paper  on the possibility of decoherence-free design of quantum gates mediated by Rydberg-excited neutral atoms. This quantum computing architecture utilizes atoms  trapped in optical fields, e.g., in optical lattices. In order to reduce motional dephasing we determine trapping conditions where AC Stark shifts of both ground and Rydberg levels are the same (so-called magic trapping).

 

 

 

Intensity landscape and the possibility of magic trapping of alkali Rydberg atoms in infrared optical lattices, T. Topcu and A. Derevianko, arxiv.org:1305.6570

Motivated by compelling advances in manipulating cold Rydberg  atoms in optical traps, we consider the effect of large extent of Rydberg electron wave function on trapping potentials. We find that when the Rydberg orbit lies outside inflection points in laser intensity landscape, the atom can stably reside in laser intensity maxima. Effectively, the free-electron  polarizability of Rydberg electron is modulated by intensity landscape and can accept both positive and negative values. We apply these insights to determining magic wavelengths for Rydberg-ground-state transitions for alkali atoms trapped in infrared optical lattices. We find magic wavelengths to be around 10 um, with exact values that depend on Rydberg state quantum numbers.

This result is somewhat unusual and more details can be found in this talk (link to pdf)  given at the Dresden workshop on ultracold Rydberg physics.

UPDATE: published: Phys. Rev. A 88, 043407 (2013)