Silicon-Based Electro-Optical Gyroscope Overcomes SNR Deficiencies

1. This electro-optical nano-gyroscope devised at Caltech measures just 2 mm on each side, yet provides excellent performance due to a technique that enables cancellation of a major source of errors. (Source: Ali Hajimiri/Caltech)

Their solution leverages what they denote as the “reciprocity” of passive optical networks to greatly reduce thermal fluctuations and mismatch, and thus yield superior results compared to previous approaches. Their demonstration device is capable of detecting phase shifts—a primary figure of merit for these units—that are 30 times smaller than state-of-the-art, miniature fiber-optic gyroscopes, even though the unit itself is 500 times smaller. The overall improvement in performance of optical gyroscopes is one to two orders of magnitude.

As published in Nature, their paper “Nanophotonic optical gyroscope with reciprocal sensitivity enhancement” explains the approach, which is somewhat analogous to using differential signals to cancel common-mode electrical signals. As with all optical gyros, their device uses the relativistic Sagnac effect to determine angular velocity, by measuring the relative phase-shifting between two counterrotating optical waves (one as a reference path, the other as signal path) created via a beam splitter from a single source. These are then recombined after their transit. When the reference frame of the gyroscope is rotating, the effective path lengths as seen by the two beams change, and thus fringing occurs between the light beams at the receiving-end sensors.

Overall performance is normally closely linked to the path length, with a longer path offering greater precision and less sensitivity to dynamic differences between the two paths. Miniaturizing the path by using a waveguide in a silicon substrate rather than lengths of optical fibers or a vacuum path means increased sensitivity to any path-related changes.

2. The optical gyro and the Sagnac effect: The silicon nanophotonic waveguide supports a single mode at 1550 nm (a); rotation of the ring induces a phase difference between the two counterrotating waves (b); in the reciprocal sensitivity enhancement technique, the incoming signal is switched between the red path (clockwise propagation) and the blue path (anticlockwise propagation). (Source: Ali Hajimiri/Caltech)

To work around this issue, the Caltech team set used a design that continually alternates the optical paths (Fig. 2) at a rate much higher than any fluctuations. The “polarity” of the signals that travel through the silicon’s optical waveguides is reversed, while undesirable common-mode components such as thermal-based fluctuations and mismatch, are attenuated. In this context, "reciprocal" means that both beams of light within the gyroscope optical waveguides are affected in the same way by imperfections.

The overall design uses a significant amount of electronics, of course, including a pair of channels comprised of photodiodes, transimpedance amplifiers (TIAs), and variable gain amplifiers (VGAs), plus low-pass filtering and demodulation (Fig. 3).

3. The input Mach-Zehnder interferometer used for path switching and the measured power in each direction versus injected current into one of the photodiodes (a). A schematic of the implemented nano-optical gyro (b). The optical signals are each captured by a photodiode, and amplified by a TIA and VGA signal chain, then added together and multiplied by the reference frequency through a passive mixer to extract the amplitude information that encodes the rate of rotation (c). (Source: Ali Hajimiri/Caltech)

The all-integrated optical gyroscope device fabricated by the researchers, headed by Ali Hajimiri, Bren Professor of Electrical Engineering and Medical Engineering in the Division of Engineering and Applied Science at Caltech, measures just 2 × 2 mm. The team maintains that their reciprocal sensitivity approach has greater benefits and much lower complexity than alternatives such as using a non-coherent light source, or employing a low-loss waveguide (which usually requires different, harder-to-fabricate optical-waveguide core and clad materials). Further, it enables detection of the smallest recorded phase-shift (just 3 nanoradians) of all miniaturized approaches implemented in silicon nanophotonics thus far.