Typical EIT level configurations.
Unlike typical EIT experiments, which utilize alkali vapor cell (typically Rb), we are currently (in collaboration with the Katz group at the Hebrew University) constructing an experimental realization of EIT in a metastable neon cell. Whereas in the alkali experiments, noble gases are typically used as a “buffer” gas to cool the alkali atoms, in our case, we expect the ground state neon atoms to act as a buffer gas to the metastable atoms. An additional benefit to using neon is that for the even (and more common) neon isotopes (20 and 22) the optical transition we will probe is a closed transition, so that we expect no radiative losses to states other then the ground state (we expect the metastable state lifetime to be on the order of 100s of ms, and are currently measuring it as a function of pressure).
A picture of our EIT cell, the plasma is generated by RF excitation, some of the electrons
in the plasma are recaptured into the metastable state. This is not Neon yet, the blue glow
is characteristic of the nitrogen in the residual air in the cell.
Recently we’ve also started discussing the complementary process, Electromagnetically Induced Absorption (EIA) in which the absorption of a beam is enhanced in the medium by the interaction with the pump beam. We are currently working on an experiment to measure both processes and transition between them. We are also looking into magnetometry using the neon atoms, by detecting Faraday rotation in the neon vapor induced by external magnetic fields.