In the pursuit of realizing quantum optical networks, a large variety of different approaches have been studied to achieve a single photon source on-demand. The common goal for these approaches is to harvest all the emission from a quantum emitter into a single spatial optical mode while maintaining a high signal-to-noise ratio. In this work, we use a single nitrogen vacancy center in diamond as a quantum emitter operating at ambient conditions and we demonstrate an increased photon count rate up to a factor of 1.76 by placing a silver mirror fabricated on the end facet of an optical fiber near the emitter.
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INTRODUCTIONIn recent years, the negatively charged nitrogen vacancy (NV) center in diamond has become one of the most attractive solid state quantum emitters due its robustness, stable emission and optically detected magnetic resonance (ODMR). By exploiting the quality of the NV center, several fundamental phenomena like spin-spin entanglement and detection of quantum coherent evolution of spin states have been demonstrated [1][2][3][4]. This enables the construction of a basic quantum spin register which is an important step towards the construction of a large scale quantum network. Furthermore, due to its atomic confinement and its long spin coherence time under ambient conditions the single NV center constitutes an excellent magnetic field sensor both in terms of sensitivity and spatial resolution. Besides the spin coherence time, the sensitivity of an NV center as a magnetic field sensor is ultimately arXiv:1406.3955v1 [quant-ph] 16 Jun 2014 2 limited by the amount of detected photons [5][6][7] and thus a high optical collection rate is of high importance.Different methods have been proposed to increase the photon collection rate from an NV center. These approaches include, among others, the placement of the NV center in a nanocavity directly processed into the diamond host material [8], micro-pillar structures [9,10], and solid immersion lenses (SILs) [11]. In a standard bulk diamond host material with an index of refraction of n D = 2.42, most of the light emitted by an NV center remains inside the diamond due to total internal reflection. This limitation could be overcome by placing detectors on the side of the diamond sample [12], where a 100-times increased signal could be obtained compared to the standard approach with a confocal microscope. Another approach to increase the photon collection rate is to place the emitter at or close to the field maximum of a waveguide mode, such that emission predominantly occurs into the guided mode. This has been shown experimentally for both dielectric [13,14] and plasmonic [15][16][17] waveguides.Another approach to increase the photon collection rate is to place a metallic mirror in close vicinity of the emitter [18]. This modifies the angular emission pattern of the emitter and changes the spontaneous decay rate, as originally demonstrated for Eu + ions [19,20] and very recently for single NV centers [21].In this article we report on an increase...