2008
DOI: 10.1103/physrevlett.101.190504
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Single-Photon Excitation of Surface Plasmon Polaritons

Abstract: We provide the quantum-mechanical description of the excitation of surface plasmon polaritons on metal surfaces by single photons. An attenuated-reflection setup is described for the quantum excitation process in which we find remarkably efficient photon-to-surface plasmon wave-packet transfer. Using a fully quantized treatment of the fields, we introduce the Hamiltonian for their interaction and study the quantum statistics during transfer with and without losses in the metal.

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Cited by 92 publications
(102 citation statements)
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“…At the quantum limit, there have been experimental demonstrations of the excitation of surface plasmons by single photon emitters. Importantly, these experiments reveal that the radiative decay of a plasmon excited by a single photon also yields a single photon, even though a surface plasmon is a collective phenomenon consisting of the in-phase oscillations of a large number of electrons [54][55][56][57][58]. Active plasmonic devices including those with gain have been reviewed elsewhere [59].…”
Section: Emitters and Detectors For Integrated Plasmonicsmentioning
confidence: 99%
“…At the quantum limit, there have been experimental demonstrations of the excitation of surface plasmons by single photon emitters. Importantly, these experiments reveal that the radiative decay of a plasmon excited by a single photon also yields a single photon, even though a surface plasmon is a collective phenomenon consisting of the in-phase oscillations of a large number of electrons [54][55][56][57][58]. Active plasmonic devices including those with gain have been reviewed elsewhere [59].…”
Section: Emitters and Detectors For Integrated Plasmonicsmentioning
confidence: 99%
“…Indeed, such a change is well known when light-matter scattering and absorption processes are involved [71]. Taking a simple linear loss model with uncorrelated Markovian noise 1 , we expect that for number states |n , the quantum observables that make up g (2) transform the numerator of eq 4.1 as n(n − 1) → η 2 n(n − 1) and the denominator as n → ηn, where η is the total loss over the length of the waveguide [83]. Thus, for this particular loss model, the second-order quantum coherence should remain unchanged.…”
Section: Characterization Of the Effects Of Loss On The Quantum Statimentioning
confidence: 99%
“…Using the relationb(t) = (2π) −1/2 dωe −iωtb (ω), the mean SPP flux at space-time coordinate (x, t) can be calculated, f out (x, t) = b † out (x, t)b out (x, t) . For a narrow wavepacket centered at ω 0 , we have [42] …”
Section: Propagation and Damping Modelmentioning
confidence: 99%