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Bulletin of the American Physical Society

Enhanced Sensitivity in a Superluminal Single Mode DPAL Cavity at Room Temperature

Tony Abi-Salloum, Joshua Yablon, Shih Tseng, M. S. Shahriar

Published Jun 6, 2012• 0 citations
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SUPERLUMINAL AND ULTRA-SLOW LIGHT PROPAGATION IN ROOM-TEMPERATURE SOLIDS

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We present for the first time cavity-controlled fluorescence spectra and decay curves of single dipole emitters interacting at room temperature with the first longitudinal mode of a Fabry-Perot microcavity offering a lambda/2-spacing between its silver mirrors. The spontaneous emission rate of individual dye molecules was found to be enhanced by the Purcell effect by up to three times compared to the rate in free space, in agreement with theoretical predictions. Moreover, our new microcavity design was found to provide long-term stability and single-molecule sensitivity under ambient conditions for several months without noticeable reduction of the cavity-Q value. We consider this as a significant advance for single-photon sources operating at room temperature.
We demonstrate a cavity-enhanced room-temperature magnetic field sensor based on nitrogen-vacancy centers in diamond. Magnetic resonance is detected using absorption of light resonant with the 1042 nm spin-singlet transition. The diamond is placed in an external optical cavity to enhance the absorption, and significant absorption is observed even at room temperature. We demonstrate a magnetic field sensitivity of 2.5  nT/Hz2.5\text{ }\text{ }\mathrm{nT}/\sqrt{\mathrm{Hz}}2.5  nT/Hz​, and project a photon shot-noise-limited sensitivity of 70  pT/Hz70\text{ }\text{ }\mathrm{pT}/\sqrt{\mathrm{Hz}}70  pT/Hz​ for a few mW of infrared light, and a quantum projection-noise-limited sensitivity of 250  fT/Hz250\text{ }\text{ }\mathrm{fT}/\sqrt{\mathrm{Hz}}250  fT/Hz​ for the sensing volume of $\ensuremath{\sim}90\text{ }\text{ }\mathrm{\ensuremath{\mu}}\mathrm{m}\ifmmode\times\else\texttimes\fi{}90\text{ }\text{ }\mathrm{\ensuremath{\mu}}\mathrm{m}\ifmmode\times\else\texttimes\fi{}200\text{ }\text{ }\mathrm{\ensuremath{\mu}}\mathrm{m}$.