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Project goalsBy placing a trapped ion within an optical cavity, we can generate a coherent interaction between the ion and the cavity field. One can think of this interaction as an atom-photon interface, allowing us to transfer quantum information between light and matter. We hope to use such an interface both to explore fundamental quantum optics and to couple trapped ions to each other via a cavity-based quantum network. Specific goals for the project include:
Experimental apparatus and resultsPrevious ion-cavity experiments in Innsbruck coupled a cavity mode to the 40Ca+ quadrupole transition, which has a 1 s lifetime. It was observed that a single ion could act as a highly sensitive probe of the cavity standing wave field [1] and that the ion's position in the cavity modifies its spontaneous emission rate [2], as predicted by cavity quantum electrodynamics. Our current apparatus is designed to couple up to three ions to a cavity. The atom-cavity interaction takes place on either the 4P1/2-3D3/2 or the 4P3/2-3D5/2 40Ca+ transition, with a lifetimes of around 90 ns. This choice of transition allows us to operate in an intermediate coupling regime in which the rate of coherent atom-cavity coupling is similar to the incoherent rates of cavity and effective atomic decay. The apparatus consists of a linear Paul trap within an optical cavity under ultra-high vacuum. The cavity is 2 cm in length, with finesse of 7 x 104 at 866 nm, and can be translated in all directions with respect to the trap. We detect cavity photons on a pair of avalanche photodiodes, and we detect atomic fluorescence from the side of the cavity on a photomultiplier tube.
By coupling the cavity to the 4P1/2-3D3/2 transition of 40Ca+ and driving the 4S1/2-4P1/2 transition with a laser, we can generate vacuum-stimulated Raman transitions between the S and D states of trapped calcium ions. We have recorded spectra of these transitions in the cavity output field and have used them to map out the standing-wave structure of the atom-field coupling [3]. Recently, we have realized an efficient single-photon source by driving Raman transitions in a pulsed scheme, generating one photon within the cavity in 88±17% of all attempts [4]. Fiber cavity developmentIn parallel with the efforts described above, we are working toward a strongly coupled, fiber-based cavity which can be integrated with surface ion traps under development in our research group. This work is in collaboration with J. Reichel at ENS, Paris, who has developed these fiber cavities for atom-chip experiments with Bose Einstein condensates [5].
Project members
References[1] "Coupling a single atomic quantum bit to a high finesse optical cavity," A. B. Mundt, A. Kreuter, C. Becher, D. Leibfried, J. Eschner, F. Schmidt-Kaler, R. Blatt, Phys. Rev. Lett. 89, 103001 (2002). [2] "Spontaneous emission lifetime of a single trapped Ca+ ion in a high finesse cavity," A. Kreuter, C. Becher, G. P. T. Lancaster, A. B. Mundt, C. Russo, H. Häffner, C. Roos, J. Eschner, F. Schmidt-Kaler, R. Blatt, Phys. Rev. Lett. 92, 203002 (2004). [3] "Raman spectroscopy of a single ion coupled to a high-finesse cavity," C. Russo, H. G. Barros, A. Stute, F. Dubin, E. S. Phillips, T. Monz, T. E. Northup, C. Becher, T. Salzburger, H. Ritsch, P. O. Schmidt, R. Blatt, Appl. Phys. B 95, 205 (2009). [4] "Deterministic single-photon source from a single ion," H. G. Barros, A. Stute, T. E. Northup, C. Russo, P. O. Schmidt, R. Blatt, New J. Phys. 11, 103004 (2009). [5] "Strong atom-field coupling for Bose-Einstein condensates on a chip," Y. Colombe, T. Steinmetz, G. Dubois, F. Linke, D. Hunger, J. Reichel, Nature 450, 272 (2007). |