Ultra-sensitive temperature sensor based on PDMS filled Fabry-Perot cavity and air-bubble Fabry-Perot cavity in parallel

被引:0
|
作者
Han, Bowen [1 ]
Jiang, Chao [1 ]
Gao, Jiawei [1 ]
Gao, Ling [1 ]
Guo, Zihao [1 ]
Guo, Xiaoshan [1 ]
Li, Hong [1 ]
Sun, Simei [1 ]
机构
[1] Hubei Normal Univ, Coll Phys & Elect Sci, Hubei Engn Res Ctr Micronano Optoelect Devices & I, Hubei Key Lab Optoelect Convers Mat & Devices, Huangshi 435002, Hubei, Peoples R China
基金
中国国家自然科学基金;
关键词
Fiber temperature sensor; Fabry-Perot interferometer; Polydimethylsiloxane; Femtosecond laser pulse; Harmonic vernier effect; Vernier effect;
D O I
10.1016/j.optcom.2024.130829
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Highly sensitive fiber optic temperature sensors are designed and fabricated using the Vernier Effect (VE) and First-order Harmonic Vernier Effect (FHVE). The sensor comprises two Fabry-Perot cavities (F-P) in parallel. Single-mode fiber is fused together with a small segment of capillary, and then polydimethylsiloxane (PDMS) is filled in the capillary to form a sensing F-P cavity. The reference F-P cavity is composed of air-bubble inside the single-mode fiber etched by femtosecond laser. Two reference interferometers FPI1 and FPI2, as well as two sensing interferometers FPI3 and FPI4, were prepared using this method. The free spectral ranges (FSR) of FPI1, FPI2, FPI3, and FPI4 are 14.09 nm, 7.80 nm, 7.01 nm, and 6.48 nm, respectively. The temperature sensitivities of FPI3 and FPI4 are 2.2622 nm/degrees C and 2.4958 nm/degrees C, respectively. FPI1 and FPI2 are almost insensitive to temperature. FPI3 and FPI2 have similar FSR, and they generate traditional VE sensor in parallel, with a temperature sensitivity of 20.41 nm/degrees C, which is about 9.02 times that of FPI3. The FSR1 of FPI1 is approximately twice that of FPI3, and they generate FHVE1 in parallel. The temperature sensitivity of FHVE1 reaches -99.66 nm/degrees C, which is 44.05 times that of FPI3 and 4.88 times that of VE1. This is currently the highest known temperature sensitivity. In addition, the FSR1 of FPI1 is also approximately twice that of FPI4. Parallel connection between FPI4 and FPI1 can also generate FHVE2, but the sensitivity is only 22.17 nm/degrees C, which is 4.5 times lower than the sensitivity of FHVE1. From this, it can be seen that in FHVE, the smaller the FSR detuning (FSRr - (i+1) FSRs) between the sensing cavity and the reference cavity, the greater the amplification factor of sensitivity. The materials of the proposed sensor are cheap, easy to fabricate, and has high sensitivity. It can be used to measure temperature in environments with high sensitivity requirements.
引用
收藏
页数:11
相关论文
共 50 条
  • [41] Parallel Polydimethylsiloxane-Cavity Fabry-Perot Interferometric Temperature Sensor Based on Enhanced Vernier Effect
    Mu, Xiaoguang
    Gao, Jiale
    Yang, Yuqiang
    Wang, Ji
    Bi, Lei
    IEEE SENSORS JOURNAL, 2022, 22 (02) : 1333 - 1337
  • [42] Polarisation dynamics of a birefringent Fabry-Perot cavity
    Ejlli, A.
    Della Valle, F.
    Zavattini, G.
    APPLIED PHYSICS B-LASERS AND OPTICS, 2018, 124 (02):
  • [43] Circular anisotropy of a rotating Fabry-Perot cavity
    Boiko, DL
    OPTICS EXPRESS, 1998, 2 (09): : 397 - 403
  • [44] Multiple Layer Fabry-Perot Cavity Antennas
    Konstantinidis, Konstantinos
    Feresidis, Alexandros P.
    Hall, Peter S.
    2013 7TH EUROPEAN CONFERENCE ON ANTENNAS AND PROPAGATION (EUCAP), 2013, : 2500 - 2504
  • [45] Fabry-Perot cavity in the field of a gravitational wave
    M. V. Sazhin
    Journal of Experimental and Theoretical Physics, 1998, 86 : 220 - 225
  • [46] MEMS tunable silicon Fabry-Perot cavity
    Masson, Jonathan
    Kone, Fatou Binetou
    Peter, Yves-Alain
    OPTOMECHATRONIC MICRO/NANO DEVICES AND COMPONENTS III, 2007, 6717
  • [47] A fiber Fabry-Perot cavity with high finesse
    Hunger, D.
    Steinmetz, T.
    Colombe, Y.
    Deutsch, C.
    Haensch, T. W.
    Reichel, J.
    NEW JOURNAL OF PHYSICS, 2010, 12
  • [48] Fabry-Perot cavity in the field of a gravitational wave
    Sazhin, MV
    JOURNAL OF EXPERIMENTAL AND THEORETICAL PHYSICS, 1998, 86 (02) : 220 - 225
  • [49] FABRY-PEROT BISTABLE CAVITY OPTIMIZATION ON REFLECTION
    WHERRETT, BS
    IEEE JOURNAL OF QUANTUM ELECTRONICS, 1984, 20 (06) : 646 - 651
  • [50] DISPLACEMENT INTERFEROMETRY WITH PASSIVE FABRY-PEROT CAVITY
    Lazar, Josef
    Cip, Ondrej
    Oulehla, Jindrich
    Pokorny, Pavel
    Fejfar, Antonin
    Stuchlik, Jiri
    NANOCON 2011, 2011, : 688 - 695