Author
Listed:
- A. Goban
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- C.-L. Hung
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- S.-P. Yu
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- J.D. Hood
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- J.A. Muniz
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- J.H. Lee
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- M.J. Martin
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- A.C. McClung
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
- K.S. Choi
(Spin Convergence Research Center 39-1, Korea Institute of Science and Technology)
- D.E. Chang
(ICFO—Institut de Ciencies Fotoniques, Mediterranean Technology Park)
- O. Painter
(Institute for Quantum Information and Matter, California Institute of Technology
Thomas J. Watson, Sr., Laboratory of Applied Physics 128-95, California Institute of Technology)
- H.J. Kimble
(Norman Bridge Laboratory of Physics 12-33, California Institute of Technology
Institute for Quantum Information and Matter, California Institute of Technology)
Abstract
The integration of nanophotonics and atomic physics has been a long-sought goal that would open new frontiers for optical physics, including novel quantum transport and many-body phenomena with photon-mediated atomic interactions. Reaching this goal requires surmounting diverse challenges in nanofabrication and atomic manipulation. Here we report the development of a novel integrated optical circuit with a photonic crystal capable of both localizing and interfacing atoms with guided photons. Optical bands of a photonic crystal waveguide are aligned with selected atomic transitions. From reflection spectra measured with average atom number , we infer that atoms are localized within the waveguide by optical dipole forces. The fraction of single-atom radiative decay into the waveguide is Γ1D/Γ′≃(0.32±0.08), where Γ1D is the rate of emission into the guided mode and Γ′ is the decay rate into all other channels. Γ1D/Γ′ is unprecedented in all current atom–photon interfaces.
Suggested Citation
A. Goban & C.-L. Hung & S.-P. Yu & J.D. Hood & J.A. Muniz & J.H. Lee & M.J. Martin & A.C. McClung & K.S. Choi & D.E. Chang & O. Painter & H.J. Kimble, 2014.
"Atom–light interactions in photonic crystals,"
Nature Communications, Nature, vol. 5(1), pages 1-9, September.
Handle:
RePEc:nat:natcom:v:5:y:2014:i:1:d:10.1038_ncomms4808
DOI: 10.1038/ncomms4808
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