{"title":"基于直接由PMMA板材制成的法布里-珀罗腔的超灵敏光纤温度传感器","authors":"Cheng Peng, Chao Jiang, Rui Li, Qun Zhang, Peiji Liang, Xiaoshan Guo, Simei Sun","doi":"10.1016/j.optcom.2025.132513","DOIUrl":null,"url":null,"abstract":"<div><div>A novel ultrasensitive optical fiber temperature sensor is proposed and experimentally validated. Temperature sensing is achieved using a Fabry-Perot interferometer (FPI) manufactured directly from the thermosensitive material polymethyl methacrylate (PMMA) slab. Firstly, we used a CO<sub>2</sub> laser to ablate a micro groove on the PMMA slab, and then two single-mode fibers (SMF) with flat cut end faces are placed in the micro groove from both sides, aligning their two reflective surfaces, then the SMF on both sides are firmly fixed using ultraviolet glue to form an FPI, named FPI<sub>1</sub>. When heating FPI<sub>1</sub>, the expansion of the PMMA slab elongates the F-P cavity length in FPI<sub>1</sub>, resulting in the variation of the optical path difference of light transmitted in FPI<sub>1</sub>, causing the dip wavelength of FPI<sub>1</sub> spectrum to drift, thus achieving temperature measurement. Due to the high coefficient of thermal expansion and contraction of PMMA slab, the temperature of a single FPI<sub>1</sub> reaches 13.35 nm/°C. To further amplify the temperature sensitivity of FPI<sub>1</sub>, we introduced optical vernier effect technology to construct sensor S<sub>1</sub>. FPI<sub>1</sub> and FPI<sub>2</sub> are paralleled to form S<sub>1</sub>. FPI<sub>2</sub> is fabricated by sequentially fusion splicing SMF - capillary - SMF, and its free spectral range is close to that of FPI<sub>1</sub>. FPI<sub>2</sub> has low temperature sensitivity and is acted as the reference interferometer in S<sub>1</sub>. The experimental findings display that the sensitivity of S<sub>1</sub> reaches 115.67 nm/°C, which is the highest temperature sensitivity currently known. It has developed the temperature sensitivity of FPI<sub>1</sub> by nearly 8.7 times. In summary, the proposed sensor has a simple structure, easy producing, low cost, robustness, and highly sensitive, making it one of the optimal choices for temperature measurement in industrial applications.</div></div>","PeriodicalId":19586,"journal":{"name":"Optics Communications","volume":"596 ","pages":"Article 132513"},"PeriodicalIF":2.5000,"publicationDate":"2025-09-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Ultra sensitive fiber optic temperature sensor based upon Fabry-Perot cavity directly fabricated from PMMA slab\",\"authors\":\"Cheng Peng, Chao Jiang, Rui Li, Qun Zhang, Peiji Liang, Xiaoshan Guo, Simei Sun\",\"doi\":\"10.1016/j.optcom.2025.132513\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>A novel ultrasensitive optical fiber temperature sensor is proposed and experimentally validated. Temperature sensing is achieved using a Fabry-Perot interferometer (FPI) manufactured directly from the thermosensitive material polymethyl methacrylate (PMMA) slab. Firstly, we used a CO<sub>2</sub> laser to ablate a micro groove on the PMMA slab, and then two single-mode fibers (SMF) with flat cut end faces are placed in the micro groove from both sides, aligning their two reflective surfaces, then the SMF on both sides are firmly fixed using ultraviolet glue to form an FPI, named FPI<sub>1</sub>. When heating FPI<sub>1</sub>, the expansion of the PMMA slab elongates the F-P cavity length in FPI<sub>1</sub>, resulting in the variation of the optical path difference of light transmitted in FPI<sub>1</sub>, causing the dip wavelength of FPI<sub>1</sub> spectrum to drift, thus achieving temperature measurement. Due to the high coefficient of thermal expansion and contraction of PMMA slab, the temperature of a single FPI<sub>1</sub> reaches 13.35 nm/°C. To further amplify the temperature sensitivity of FPI<sub>1</sub>, we introduced optical vernier effect technology to construct sensor S<sub>1</sub>. FPI<sub>1</sub> and FPI<sub>2</sub> are paralleled to form S<sub>1</sub>. FPI<sub>2</sub> is fabricated by sequentially fusion splicing SMF - capillary - SMF, and its free spectral range is close to that of FPI<sub>1</sub>. FPI<sub>2</sub> has low temperature sensitivity and is acted as the reference interferometer in S<sub>1</sub>. The experimental findings display that the sensitivity of S<sub>1</sub> reaches 115.67 nm/°C, which is the highest temperature sensitivity currently known. It has developed the temperature sensitivity of FPI<sub>1</sub> by nearly 8.7 times. In summary, the proposed sensor has a simple structure, easy producing, low cost, robustness, and highly sensitive, making it one of the optimal choices for temperature measurement in industrial applications.</div></div>\",\"PeriodicalId\":19586,\"journal\":{\"name\":\"Optics Communications\",\"volume\":\"596 \",\"pages\":\"Article 132513\"},\"PeriodicalIF\":2.5000,\"publicationDate\":\"2025-09-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Optics Communications\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0030401825010417\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optics Communications","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0030401825010417","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"OPTICS","Score":null,"Total":0}
Ultra sensitive fiber optic temperature sensor based upon Fabry-Perot cavity directly fabricated from PMMA slab
A novel ultrasensitive optical fiber temperature sensor is proposed and experimentally validated. Temperature sensing is achieved using a Fabry-Perot interferometer (FPI) manufactured directly from the thermosensitive material polymethyl methacrylate (PMMA) slab. Firstly, we used a CO2 laser to ablate a micro groove on the PMMA slab, and then two single-mode fibers (SMF) with flat cut end faces are placed in the micro groove from both sides, aligning their two reflective surfaces, then the SMF on both sides are firmly fixed using ultraviolet glue to form an FPI, named FPI1. When heating FPI1, the expansion of the PMMA slab elongates the F-P cavity length in FPI1, resulting in the variation of the optical path difference of light transmitted in FPI1, causing the dip wavelength of FPI1 spectrum to drift, thus achieving temperature measurement. Due to the high coefficient of thermal expansion and contraction of PMMA slab, the temperature of a single FPI1 reaches 13.35 nm/°C. To further amplify the temperature sensitivity of FPI1, we introduced optical vernier effect technology to construct sensor S1. FPI1 and FPI2 are paralleled to form S1. FPI2 is fabricated by sequentially fusion splicing SMF - capillary - SMF, and its free spectral range is close to that of FPI1. FPI2 has low temperature sensitivity and is acted as the reference interferometer in S1. The experimental findings display that the sensitivity of S1 reaches 115.67 nm/°C, which is the highest temperature sensitivity currently known. It has developed the temperature sensitivity of FPI1 by nearly 8.7 times. In summary, the proposed sensor has a simple structure, easy producing, low cost, robustness, and highly sensitive, making it one of the optimal choices for temperature measurement in industrial applications.
期刊介绍:
Optics Communications invites original and timely contributions containing new results in various fields of optics and photonics. The journal considers theoretical and experimental research in areas ranging from the fundamental properties of light to technological applications. Topics covered include classical and quantum optics, optical physics and light-matter interactions, lasers, imaging, guided-wave optics and optical information processing. Manuscripts should offer clear evidence of novelty and significance. Papers concentrating on mathematical and computational issues, with limited connection to optics, are not suitable for publication in the Journal. Similarly, small technical advances, or papers concerned only with engineering applications or issues of materials science fall outside the journal scope.