Download Engineering the Atom-Photon Interaction: Controlling by Ana Predojević, Morgan W. Mitchell PDF

By Ana Predojević, Morgan W. Mitchell

This booklet presents a complete view of the modern tools for quantum-light engineering. particularly, it addresses diversified technological branches and hence permits the reader to fast establish the easiest expertise - program fit. Non-classical gentle is a flexible device, confirmed to be an intrinsic a part of a number of quantum applied sciences. Its ancient importance has made it the topic of many textual content books written either from theoretical and experimental perspective. This publication takes one other point of view by means of giving an perception to fashionable applied sciences used to generate and control quantum light.

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Additional info for Engineering the Atom-Photon Interaction: Controlling Fundamental Processes with Photons, Atoms and Solids

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E. the probability for correlations between the two detectors monitoring the beam-splitter output depends strongly on the timing of the photo detections. For instance, the coincidence probability P(Ci , Dj ) for detector C clicking in time bin i and detector D in time bin j is then P(Ci , Dj ) ∝ sin2 ((φi − φj )/2). 33) 28 A. Kuhn We have been exploring these phenomena [81] with the experiment illustrated in Fig. 11, using two types different signal photons. e. φ1 = φ2 = φ3 = 0, and the other with φ1 = 0, φ2 = π, φ3 = 0.

A photon turnstile dynamically regulated by one atom. Science 319, 1062–1065 (2008) 52. T. , Efficient routing of single photons by one atom and a microtoroidal cavity. Phys. Rev. Lett. 102, 083601 (2009) 53. M. Pöllinger, D. O’Shea, F. Warken, A. Rauschenbeutel, Ultrahigh-Q tunable whisperinggallery-mode microresonator. Phys. Rev. Lett. 103, 053901 (2009) 54. A. , Step by step engineered many particle entanglement. Science 288, 2024 (2000) 55. A. , Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics.

G. photonic time bin or polarisation encoded qubits [17, 45, 86]. Prior to investigating the effect of the atom-cavity and atom-laser coupling, we briefly revisit the input-output coupling of an optical cavity in the time domain (Fig. 12). Inside the cavity, we assume that the mode spacing is so large that only one single mode of frequency ωcav contributes, with the dimension-less probability amplitude ccav (t) determining the occupation of the one-photon Fock state |1 . Furthermore, we assume that coupling to the outside field is fully controlled by the field reflection and transmission coefficients, r and τ , of the coupling mirror, while the other has a reflectivity of 100 %.

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