The integrated optical gyroscope is a highly possible way to achieve chip-level gyroscopes. We proposed and simulated a three-dimensional Si3N4 optical interconnect platform. It transforms the waveguide coil from a single-layer structure to a multi-layer structure, which can increase the sensing area of the coil under the same footprint. The proposed platform with low interlayer transition loss and crossing loss can reduce the overall loss in the coil and improve the theoretical angular random walk (ARW). A quadruple-layer sensing coil with a maximum radius of 30 mm and a total length of 2.08 m is derived, which can attain an ARW of 0.15 deg/√h and an insertion loss of 3.15 dB in theory.
Gyroscope is a sensor that measures angular velocity, which is widely used in precision guidance, deep-sea operations, unmanned driving, etc. Currently, the gyroscope is moving towards the trend of compactness, high accuracy, high reliability and low cost, and the resonance integrated optical gyroscope is expected to be a preferred choice for the next generation of optical gyroscopes. In this paper, the finite element method is used for modeling and numerical simulation of silicon-based optical waveguide micro-ring resonator, a sensitive unit of resonant integrated optical gyroscope, in two-dimensional and three-dimensional, to research the effect of structural parameters of the resonator on its performance. Simulation results show that the free spectral width of the Si-based optical waveguide micro-ring decreases with increasing radius. The resonant depth of the micro-ring increases with the coupling spacing in a certain range, but it decreases with the coupling spacing beyond the critical coupling. In addition, the quality factor of the micro-ring resonator increases with the increase of radius. The research in this paper lays the foundation for performance optimization of the resonator.
To improve the performance of differential transmissivity & reflectivity measurer (DFTRM) for coated mirrors with extremely low transmission or reflection loss, a novel scheme based on Fresnel formula and optical balance is demonstrated. Benefit from the characteristic of Fresnel formula, i.e., the specular reflectivity of the reference optical surface varies slowly with the incident angle near Brewster’s angle, so the precision measurement of transmissivity or reflectivity is then converted to the precision measurement of the incident angle in our two-optical-path scheme. An experimental system is set up to verify the feasibility of precision measurement, and the preliminary measurement results for high-reflectivity coated mirrors with low transmission loss prove its ability to measure transmissivity and distinguish the transmissivity difference of 10 parts per million (ppm) magnitude. Various potential error sources, including the responsivity of photodiodes, the scale factor, the polarization of the incident laser, the refractive index of the reference medium and the spatial relationship of components, are discussed qualitatively or quantitatively to provide guidance for the subsequent optimization of transmissivity & reflectivity measurer at ppm level in the future.
The quality of the output signal of the laser gyro is closely related to the loss of the high mirror. At present, the research on the total loss of the high-reflection film has been quite perfect. In order to further study the optical properties of the high-reflection film, the total loss of the high-reflection film can be refined into three parts: transmission loss, scattering loss and absorption loss. Starting from the current research situation at home and abroad, this paper mainly introduces three methods, including spectrophotometer method, DF transflectometer and cavity ring-down technique, and discusses the measurement principles of these three methods. The development status and accuracy level of transmittance measurement technology, and the advantages and disadvantages of these three methods are analyzed, and the methods to improve the measurement accuracy and the possible development direction in the future are pointed out. Finally, other common methods of transmittance and reflectance measurement and the corresponding measurement accuracy are introduced.
Polarizing beam splitter is designed with a broadband and wide range of incident angle. Polarizing beam splitter designed here is a kind of double periodic subwavelength medium-metal grating, which consisted of silicon dioxide as the substrate, magnesium fluoride (MgF2) as medium material and silver for the grid lines. It has the polarization splitting function of TE reflection and TM transmission. Based on the rigorous coupled-wave analysis(RCWA) and the continuous optimization of the structure parameters, the polarization beam splitter has high polarization conversion efficiency, high extinction ratio and a wide tolerance of incident angle in the near infrared band (1μm − 3μm) .The simulation results show that the reflection efficiency of TE polarized light and the transmission efficiency of TM polarized light are both higher than 96%, and the reflection extinction ratio and transmission extinction ratio are greater than 17dB and 28dB respectively. When the incident angle of incident light is from -80° to 80°, the reflection efficiency of TE polarized light is over 96%; when the incident angle is from -40°to 40°, the transmission efficiency of TM polarized light is over 90%. The reflection extinction ratio exceeds 17dB, and the transmission extinction ratio exceeds 35dB in the incident wavelength of 1550nm.The designed polarizing beam splitter is expected to be used in optical communication, optical storage, optical sensing and other fields for light modulation and control.
A nanoslit array is introduced on the silicon waveguide, and the phase difference is controlled by the slit width to satisfy the function of the focusing lens. If keep the designed width and depth of the slit in accordance with the focusing effect unchanged, when the incident wavelength changes, the focal position must change accordingly, and the dispersion effect is significant. In order to achieve the achromatic effect, the refractive index of the surrounding medium is changed while changing the wavelength. Finally, the refractive index of the surrounding medium which can keep the focal length constant at the wavelength of 1550-1950nm is obtained, and the equation that the change of the refractive index and the wavelength of the medium makes the focal length constant is obtained. The achromatic effect can be effectively achieved, and applications range of achromatic metalens from imaging in optical communications to telescopes in the astronomical field.
We introduce phase-change material Ge2Sb2Te5 (GST) into metal–insulator–metal (MIM) waveguide systems to realize chipscale plasmonic modulators and switches in the telecommunication band. Benefitting from the high contrast of optical properties between amorphous and crystalline GST, the three proposed structures can act as reconfigurable and nonvolatile modulators and switches with excellent modulation depth 14 dB and fast response time in subnanosecond while possessing small footprints, simple frameworks, and easy fabrication. We provide solutions to design active devices in MIM waveguide systems and can find potential applications in more compact all-optical circuits for information processing and storage.
Metamaterials have attracted a lot of attention in the past decade, because of its remarkable properties in electronics and photonics. Recently, a new kind of two-dimensional metamaterial named metasurface have led the research front. Metasurfaces show up excellent optical properties by patterning planar nanostructures. Novel optical phenomena based on graphene include ultra-thin focusing, anomalous reflection or refraction strong spin-orbit and so on. In this work, we have designed a novel infrared light polarized beam splitter by combining the 2D array of graphene with a subwavelength-thickness optical cavity, which demonstrated great splitting effect in infrared wavelength. Our demonstration pave a novel way for the infrared light polarized beam splitting.
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