2011
DOI: 10.1364/oe.19.002440
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Controlled generation of single photons in a coupled atom-cavity system at a fast repetition-rate

Abstract: We have demonstrated high-speed controlled generation of single photons in a coupled atom-cavity system. A single 85Rb atom, pumped with a nanosecond-pulse laser, generates a single photon into the cavity mode, and the photon is then emitted out the cavity rapidly. By employing cavity parameters for a moderate coupling regime, the single-photon emission process was optimized for both high efficiency and fast bit rates up to 10 MHz. The temporal single-photon wave packet was studied by means of the photon-arriv… Show more

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Cited by 10 publications
(8 citation statements)
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“…Both effects facilitate the generation and efficient collection of single photons and, thus, the study of the Purcell effect has been extended to multiple types of emitters. These include atoms [4,5], quantum dots [6,7], and a variety of other solid-state systems [8][9][10][11] amongst others, with particular emphasis on the development of single-photon sources (SPS) [12][13][14][15][16][17][18]. The required high cooperativities can be obtained by tailoring the resonator, i.e.…”
mentioning
confidence: 99%
“…Both effects facilitate the generation and efficient collection of single photons and, thus, the study of the Purcell effect has been extended to multiple types of emitters. These include atoms [4,5], quantum dots [6,7], and a variety of other solid-state systems [8][9][10][11] amongst others, with particular emphasis on the development of single-photon sources (SPS) [12][13][14][15][16][17][18]. The required high cooperativities can be obtained by tailoring the resonator, i.e.…”
mentioning
confidence: 99%
“…The frequency of the repumping laser (ECDL 2) is fixed on resonance to the to transition, 780.232684(2) nm (384.234683(1) THz). Given a magnetic field gradient of 7.9 G/cm, the atoms are successfully trapped about 6 mm above a high-finesse optical cavity [ 35 , 36 , 37 ]. Figure 5 b shows a MOT fluorescence taken with an electron multiplying (EM) CCD, through a lens system with a numerical aperture of 0.23.…”
Section: Resultsmentioning
confidence: 99%
“…The cooling laser (ECDL 1) frequency is locked at 780.246031( 2 on resonance to the F = 1 to F = 2 transition, 780.232684(2) nm (384.234683(1) THz). Given a magnetic field gradient of 7.9 G/cm, the atoms are successfully trapped about 6 mm above a high-finesse optical cavity [34][35][36]. Fig.…”
Section: F Application To Cold Atom Experimentsmentioning
confidence: 99%