2019
DOI: 10.1007/978-3-319-98402-5_3
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Nonlinear Interactions and Non-classical Light

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Cited by 16 publications
(18 citation statements)
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“…In summary, we demonstrated EIT-based LSR and SLPs for weak coherent light pulses containing as low asn = 1.1(2) photons per pulse, implemented in a medium of cold atoms inside a HCPBGF. We observed a LSR and SLP efficiency of up to 0.36(4) and 0.16 (2), respectively, with an unconditional noise floor ofn noise = 0.017(4) photons per pulse. This was enabled, amongst others, by a careful characterization of a strongly birefringent HCPBGF, resulting in an efficient suppression of noise.…”
Section: Discussionmentioning
confidence: 89%
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“…In summary, we demonstrated EIT-based LSR and SLPs for weak coherent light pulses containing as low asn = 1.1(2) photons per pulse, implemented in a medium of cold atoms inside a HCPBGF. We observed a LSR and SLP efficiency of up to 0.36(4) and 0.16 (2), respectively, with an unconditional noise floor ofn noise = 0.017(4) photons per pulse. This was enabled, amongst others, by a careful characterization of a strongly birefringent HCPBGF, resulting in an efficient suppression of noise.…”
Section: Discussionmentioning
confidence: 89%
“…This small signal in addition is delayed with respect to the switch-off time of the backward control field. The delayed read-out can be well-explained by considering the SLP group velocity v SLP gr = v gr cos 2φ with tan 2 [48]. For Ω − c /Ω + c = 1.84 the SLP propagates backward at around −0.55 × v gr during ∆t SLP and thus exits the medium at later times during the retrieval in the forward direction.…”
Section: Stationary Light Pulsesmentioning
confidence: 99%
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“…Let H be an infinite dimensional (complex) Hilbert space, with orthonormal basis {|n } n∈N0 . This could for example be the space corresponding to a single mode of the electro-magnetic field [50]. For simplicity we consider X = R and define the feature map ϕ : R → H as…”
Section: Coherent States and Gaussian Kernelmentioning
confidence: 99%
“…Coherent states are commonly considered the most classical states in quantum optics, and are easy to simulate on a classical device. Working with a quantum device becomes interesting when the states become nonclassical [50]. When using the coherent feature map (19), the embedding of a sample (11) corresponds to the so-called cat-states [13,38,39].…”
Section: Coherent States and Gaussian Kernelmentioning
confidence: 99%