G. Rempe (P3b MPQ), colloquium, From Quantum Interconnects to Quantum Internets
E. Figueroa (P3b MPQ), talk, A single-atom quantum memory
G. Rempe (P3b MPQ), talk, Hybrid Quantum Systems and Interconnects
G. Rempe (P3b MPQ), seminar, Entanglement Distribution between Atomic Systems
C. Nölleke (P3b MPQ), talk, A Single-Atom Quantum Memory
H. Chibani (P3b MPQ), poster, A new cavity QED apparatus at work
M. Martinez-Dorantes (P6 UBONN), poster, Towards photon storage in small atomic ensembles using optical fiber Fabry-Perot Resonators
Th. Schumm (P12 TUWIEN), invited talk, Non-linear atom optic with artom chips
C. Sames (P3b MPQ), talk, FPGA-based Feedback Control of a Single Atom Trajectory
Physical Review Letters 105, 173003 (2010)
doi: 10.1103/PhysRevLett.105.173003
We demonstrate feedback cooling of the motion of a single rubidium atom trapped in a high-finesse optical resonator to a temperature of about 160 μK. Time-dependent transmission and intensity-correlation measurements prove the reduction of the atomic position uncertainty. The feedback increases the 1/e storage time into the 1 s regime, 30 times longer than without feedback.
Nature 474, 623 (2011)
doi:10.1038/nature10170
Single quantum emitters such as atoms are well known as non-classical light sources with reduced noise in the intensity, capable of producing photons one by one at given times. However, the light field emitted by a single atom can exhibit much richer dynamics. A prominent example is the predicted ability of a single atom to produce quadrature-squeezed light, which has fluctuations of amplitude or phase that are below the shot-noise level. However, such squeezing is much more difficult to observe than the emission of single photons.
Applied Physics B 102, 433 (2011)
doi: 10.1007/s00340-011-4410-x
We discuss feedback control of the motion of a single neutral atom trapped inside a high-finesse optical cavity. Based on the detection of single photons from a probe beam transmitted through the cavity, the position of the atom in the trap is estimated. Following this information, the trapping potential is switched between a high and a low value in order to counteract the atomic motion. This allowed us to increase the storage time by about one order of magnitude.