Laser & Optoelectronics Progress, Volume. 56, Issue 17, 170620(2019)
Characteristics and Sensing Applications of Few-Mode Fiber with Critical Wavelength
Fig. 1. Diagram of the FMF cross-section structure. (a) Geometrical structure and relative refractive index difference profile; (b) scanning electron microscope micrograph
Fig. 3. Simulation curves of the propagation constant difference Δβ of LP01 and the LP02 modes propagating in the FMF, and the transmission spectrum of the SFS structure (LFMF=50 cm) under the temperature of 25 ℃ versus wavelength
Fig. 4. Simulation curves of the propagation constant difference Δβ of the LP01 and LP02 modes propagating in the FMF, and the transmission spectra of the SFS structure (LFMF=16 cm) versus wavelength when temperature changes. (a) Δβ without thermal stress; (b) Δβ with thermal stress; (c) transmission spectra without thermal stress;(d) transmission spectra with thermal stress
Fig. 5. Experimental transmission spectra of the SFS structure (LFMF=16 cm) and critical wavelength shifts when temperature changes. (a) Experimental transmission spectra of the SFS structure; (b) critical wavelength shift versus temperature
Fig. 6. Transmission spectra of the SFS structure (LFMF=50 cm) versus temperature
Fig. 7. Simulated and experimental results of temperature sensitivity of the interference fringes in the transmission spectrum of the SFS structure
Fig. 8. Simulation curves of propagation constant difference Δβ of the LP01 and LP02 modes propagating in the FMF under axial strain variation
Fig. 9. Results of experimental measurements. (a) Transmission spectra of the SFS structure (LFMF=30 cm) under axial strain variation; (b) critical wavelength shift of CWL versus axial strain
Fig. 10. Relationship between axial strain sensitivity of the interference fringes in the transmission spectrum of the SFS structure and normalized wavelength
Fig. 11. Output of sensor containing the SFS structure (LFMF=20 cm) varies with temperature and axial strain. (a) Wavelength shifts for PH, 1 and PL, 1 over a 30-min period of the experiment; (b) curves of the applied and calculated axial strains over that time; (c) curves of the applied and calculated temperatures
Fig. 12. Sensor outputs of the polyimide-coated SFS structure (LFMF=15 cm) under relative humidity variation. (a) Transmission spectra; (b) wavelength shifts of interference dips DL, 1, DL, 2, DL, 3, and DL, 4
Fig. 13. Simulation of the propagation constant difference Δβ of LP01 and LP02 modes, and the transmission spectra of the SFS structure (LFMF=35 cm) versus wavelength with different equivalent curvatures of the FMF
Fig. 14. Experimental results of the transmission spectra of the SFS structure (LFMF=35 cm) versus wavelength with different curvatures of the FMF
Fig. 15. Simulation and experimental results of the critical wavelength shift versus equivalent curvature of the FMF
Fig. 16. Displacement sensor with large measurement range based on the SFS structure (LFMF=10 cm). (a) Experimental diagram; (b) experimental setup; (c) geometrical mathematical model of circular helix
Fig. 17. Large displacement sensor based on the SFS structure (LFMF=10 cm). (a) Transmission spectra under different displacements; (b) change of the FMF equivalent curvature and shifts of the critical wavelengths under displacement variation
Fig. 18. Simulation of the critical wavelength shifts in the transmission spectra of the etched SFS structure with different dFMF. The inset is the simulation of the propagation constant difference of the LP01 and LP02 modes versus wavelength with different dFMF
Fig. 19. Transmission spectra of the etched SFS structure (LFMF=20 cm, dFMF=21.3 μm) under different SRIs. (a) SRI is 1.316;(b) SRI is 1.383;(c) SRI is 1.423;(d) SRI is 1.439
Fig. 20. Experimental results (marked with error bars) of the critical wavelength shift in the transmission spectrum of the etched SFS structure under surrouding refractive index variation
Fig. 21. Simulation of the transmission spectra of the etched SFS structure (dFMF=21.3 μm, LFMF=20 cm) and shifts of the critical wavelength and the interference peaks/dips under surrounding refractive index variation. (a) Shifts of the critical wavelength and the interference peaks/dips (DL,1, PL,1, PH,1, DH,1) on each side of the critical wavelength; (b) transmission spectra under the SRIs of 1.350, 1.355, and 1.360
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Chenxu Lu, Xiaopeng Dong, Juan Su, Xueqin Lei. Characteristics and Sensing Applications of Few-Mode Fiber with Critical Wavelength[J]. Laser & Optoelectronics Progress, 2019, 56(17): 170620
Category: Fiber Optics and Optical Communications
Received: May. 5, 2019
Accepted: Jun. 6, 2019
Published Online: Sep. 5, 2019
The Author Email: Xiaopeng Dong (xpd@xmu.edu.cn)