2013
DOI: 10.1088/2040-8978/15/5/055403
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A tunable polarization-independent comb filter based on high-order mode fiber

Abstract: This paper presents an all-fiber tunable comb filter based on high-order mode fiber (HOMF). The filter is constructed by splicing a segment of HOMF between two sections of conventional single-mode fibers (SMFs), with an intentionally introduced offset at the first joint between the SMF and HOMF, and without an offset at the second joint between the HOMF and SMF, to optimize the visibility of the transmission spectrum. The optimal transverse offset of the fibers at the first joint and the tunable polarization-i… Show more

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Cited by 14 publications
(5 citation statements)
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“…×°∂ is the thermal expansion coefficient for pure silica. To calculate Equation 6 Combing Equations (5) and (6), the temperature wavelength senstivitiy of the peaks, / T λ ∆ ∆ , as a function of wavelength, is thus given by Equation (7). As shown in Equation 7, with specified fiber parameters and structures shown in Fig.…”
Section: Temperature Sensitivies Of Peaksmentioning
confidence: 99%
See 1 more Smart Citation
“…×°∂ is the thermal expansion coefficient for pure silica. To calculate Equation 6 Combing Equations (5) and (6), the temperature wavelength senstivitiy of the peaks, / T λ ∆ ∆ , as a function of wavelength, is thus given by Equation (7). As shown in Equation 7, with specified fiber parameters and structures shown in Fig.…”
Section: Temperature Sensitivies Of Peaksmentioning
confidence: 99%
“…With advantages of their high sensitivity, immunity to electromagnetic interference, compact size and durability in harsh and corrosive environments, the in-line MZIs based on two modes interference have been applied to various industrial circumstances, such as structural health monitoring, earthquake monitoring and manufacturing, for example [4][5][6]. For most reported in-line MZIs based on two modes interference, because the propagation constant difference between two interference modes change linearly with wavelength, the interference fringes, which have been seen in the transmission spectra, change periodically and the peaks/dips shift in the same wavelength direction under different strain or temperature variations [1][2][3]7]. However, in some modal interferometers based on the interference between the fundamental core mode, LP01, and the first circularly symmetric higher-order core mode, LP02, a critical wavelength (CWL) exists in the transmission spectra, and the wavelength spacing between adjacent peaks reach a maximum for the peak that closest to CWL on each side.…”
Section: Introductionmentioning
confidence: 99%
“…close to the CWL, whether on the left or right side [14]. Previous studies by some of the authors [12][13][14][15] indicate that an exclusive value of the CWL may exist in the transmission spectrum of a SFS structure employing a specially designed FMF, which supports only two modes, LP01 and LP02 [16] and the interference between these two modes may produce a stable and polarization-independent transmission spectrum [17]. The peaks closest to the CWL on each side exhibit maximum strain/temperature sensitivities and they shift in opposite directions, with different strain/temperature sensitivities.…”
mentioning
confidence: 99%
“…This is different from the conventional few mode fiber approach, in which several higher order core modes (e.g., LP11) are supported. Here the DMF used in this sensor structure is superior in its polarization behavior [24] and it is stable, even with the variation of the contaminants experienced in the underwater environment. As reported in our previous work [25], the propagation constant difference between the LP01 and the LP02 modes, Δβ, has a maximum corresponding to the critical wavelength (CWL) in the transmission spectrum.…”
Section: Introductionmentioning
confidence: 99%