Martino De Carlo, F. De Leonardis, F. Dell’Olio, Pietro Peliti, Fabrizio Berton, Mario Lucchesini, V. Passaro
{"title":"反宇称时间对称陀螺仪的间接耦合光学谐振器","authors":"Martino De Carlo, F. De Leonardis, F. Dell’Olio, Pietro Peliti, Fabrizio Berton, Mario Lucchesini, V. Passaro","doi":"10.1109/INERTIAL53425.2022.9787722","DOIUrl":null,"url":null,"abstract":"Optical gyroscopes, which exploit the Sagnac effect, are one of the preferred choices for high-resolution sensing of angular velocity. However, their miniaturization and integration for high-resolution sensing is still a challenge in optoelectronics research. In fact, in interferometric fiber-optic gyroscopes (IFOGs) the sensitivity is proportional to the area enclosed by the fiber-optic sensing coil. Whereas, in resonant fiber-optic gyroscopes (RFOGs) and resonant micro-optical gyroscopes (RMOGs) the sensitivity is proportional to the ratio between the area enclosed by the cavity and the perimeter of the cavity. Non-Hermitian optical architectures (especially with parity-time-symmetric Hamiltonians) have been recently proposed in literature to solve this scaling problem. In this work, an anti-parity-time-symmetric gyroscope has been designed with two resonant cavities, indirectly coupled via an auxiliary bus. At the operating condition of the so-called \"exceptional point\", it is possible to demonstrate that the sensitivity of the gyroscope is independent of the dimensions of the device. Finally, it will be shown that the anti-parity-time-symmetric architectures represent a better choice for angular velocity sensing than the parity-time symmetric version. An enhancement of the sensitivity of several orders of magnitude with respect to standard Sagnac-based gyros with the same footprint is expected.","PeriodicalId":435781,"journal":{"name":"2022 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)","volume":"77 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-05-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Indirectly-coupled optical resonators for anti-parity-time-symmetric gyroscopes\",\"authors\":\"Martino De Carlo, F. De Leonardis, F. Dell’Olio, Pietro Peliti, Fabrizio Berton, Mario Lucchesini, V. Passaro\",\"doi\":\"10.1109/INERTIAL53425.2022.9787722\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Optical gyroscopes, which exploit the Sagnac effect, are one of the preferred choices for high-resolution sensing of angular velocity. However, their miniaturization and integration for high-resolution sensing is still a challenge in optoelectronics research. In fact, in interferometric fiber-optic gyroscopes (IFOGs) the sensitivity is proportional to the area enclosed by the fiber-optic sensing coil. Whereas, in resonant fiber-optic gyroscopes (RFOGs) and resonant micro-optical gyroscopes (RMOGs) the sensitivity is proportional to the ratio between the area enclosed by the cavity and the perimeter of the cavity. Non-Hermitian optical architectures (especially with parity-time-symmetric Hamiltonians) have been recently proposed in literature to solve this scaling problem. In this work, an anti-parity-time-symmetric gyroscope has been designed with two resonant cavities, indirectly coupled via an auxiliary bus. At the operating condition of the so-called \\\"exceptional point\\\", it is possible to demonstrate that the sensitivity of the gyroscope is independent of the dimensions of the device. Finally, it will be shown that the anti-parity-time-symmetric architectures represent a better choice for angular velocity sensing than the parity-time symmetric version. An enhancement of the sensitivity of several orders of magnitude with respect to standard Sagnac-based gyros with the same footprint is expected.\",\"PeriodicalId\":435781,\"journal\":{\"name\":\"2022 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)\",\"volume\":\"77 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2022-05-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2022 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/INERTIAL53425.2022.9787722\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2022 IEEE International Symposium on Inertial Sensors and Systems (INERTIAL)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/INERTIAL53425.2022.9787722","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Indirectly-coupled optical resonators for anti-parity-time-symmetric gyroscopes
Optical gyroscopes, which exploit the Sagnac effect, are one of the preferred choices for high-resolution sensing of angular velocity. However, their miniaturization and integration for high-resolution sensing is still a challenge in optoelectronics research. In fact, in interferometric fiber-optic gyroscopes (IFOGs) the sensitivity is proportional to the area enclosed by the fiber-optic sensing coil. Whereas, in resonant fiber-optic gyroscopes (RFOGs) and resonant micro-optical gyroscopes (RMOGs) the sensitivity is proportional to the ratio between the area enclosed by the cavity and the perimeter of the cavity. Non-Hermitian optical architectures (especially with parity-time-symmetric Hamiltonians) have been recently proposed in literature to solve this scaling problem. In this work, an anti-parity-time-symmetric gyroscope has been designed with two resonant cavities, indirectly coupled via an auxiliary bus. At the operating condition of the so-called "exceptional point", it is possible to demonstrate that the sensitivity of the gyroscope is independent of the dimensions of the device. Finally, it will be shown that the anti-parity-time-symmetric architectures represent a better choice for angular velocity sensing than the parity-time symmetric version. An enhancement of the sensitivity of several orders of magnitude with respect to standard Sagnac-based gyros with the same footprint is expected.