We are actively looking for a long term JRF to join our group
Atom-cavity strong coupling, optical bistability and all optical switching:
We experimentally demonstrated collective strong coupling, optical bistability, and all-optical switching in a system consisting of ultracold 85Rb atoms, trapped in a dark magneto-optical trap, and coupled to an optical Fabry-Perot cavity. The collective strong coupling was established by the observation of vacuum Rabi splitting (VRS) in the transmission spectrum of an on-axis weak probe beam. A closer look at VRS measurements done with different probe light intensities showed that VRS decreases with increasing probe intensity. The measurements also revealed an asymmetry in the line shape of the vacuum-Rabi peaks – a signature of optical bistability. When the probe laser is locked to the atomic transition and its power is scanned, the cavity transmission shows bistable behaviour and the cavity input-output curve shows hysteresis. The shape of the hysteresis could be controlled by another off-axis control laser, with a few µW power (Pc ), tuned near a different atomic transition (see figure below). This results from the probe and control beams forming a Λ-type system. We also demonstrated that the cavity transmission can be switched on and off in micro-second timescales using micro-Watt control powers.
Nondestructive detection of ions by atom-cavity collective strong coupling:
We demonstrated a technique, based on atoms coupled to an optical cavity, for nondestructive detection of trapped ions. We demonstrate the vacuum-Rabi splitting (VRS), arising from collective strong coupling of ultracold Rb atoms and a cavity, to change in the presence of trapped Rb+ ions (see figure below). The Rb+ ions are optically dark and the Rb atoms are prepared in a dark magneto-optical trap. The VRS is measured on an optically open transition of the initially dark Rb atoms. The measurement itself is fast, nondestructive, and has sufficient fidelity to permit the measurement of the atomic-state-selective ion-atom collision rate. This demonstration illustrates a method based on atom-cavity coupling to measure two-particle interactions generically and nondestructively.