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Slow Light Augmented Unbalanced Interferometry for Extreme Enhancement in Sensitivity of Measuring Frequency Shift in a Laser
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We demonstrate a slow-light augmented unbalanced Mach-Zehnder Interferometer (MZI) which can be used to enhance very significantly the sensitivity of measuring the frequency shift in a laser. The degree of enhancement depends on the group index of the slow-light medium, the degree of imbalance between the physical lengths of the two arms of the MZI, and the spectral width of the laser. For a laser based on a high-finesse cavity, yielding a narrow quantum noise limited spectral width, the group index has to be larger than the finesse in order to achieve enhancement in measurement sensitivity. For the reported results, strong slow-light effect is produced by employing electro-magnetically induced transparency via coherent population trapping in a buffer-gas loaded vapor cell of Rb atoms, with a maximum group index of ~1759. The observed enhancement in sensitivity for a range of group indices agrees well with the theoretical model. The maximum sensitivity enhancement factor realized is ~560; much larger values can be obtained by using cold atoms for producing the slow-light effect. The sensitivity of any sensor that relies on measuring the frequency shift of a laser can be enhanced substantially using this technique. These include, but are not limited to, gyroscopes and accelerometers based on a conventional ring laser or a superluminal ring laser, and detectors for virialized ultra-light field dark matter.
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Cited by 2 Pith papers
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The General Quantum Limit for and the Optimization of the Minimum Measurable Frequency Shift in a Laser
MMFS of an ideal laser is the RMS of spontaneous-emission phase diffusion and vacuum shot noise; optimized UMZI, FPC, and heterodyne sensors can reach ~sqrt(measurement bandwidth times STL).
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Slow Light Augmented Fabry-Perot Cavity for Enhanced Sensitivity in Measuring Frequency Shift
A slow-light medium in a Fabry-Perot cavity multiplies the sensitivity for measuring laser frequency shifts by roughly the group index times the cavity finesse, giving a predicted enhancement up to about 1.4x10^5.
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