2020
DOI: 10.1364/oe.413139
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Analytical and experimental study on a bent abrupt taper

Abstract: This work presents an analytical coupling model for perturbed abrupt fiber tapers in single-mode fibers. In addition to LP0m modes, the modeling predicts the presence of LP11 and LP12 modes for a bent taper. Our model also introduces a perturbation function that can match most cases of bending variations on a taper. We have shown that the tapering and bending effect can be treated separately within one abstract formulation. Agreement amongst the model predictions and experimental results suppor… Show more

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Cited by 4 publications
(4 citation statements)
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“…It is worth noting that in addition to the HE 11 and LP 11 modes, other higher-order modes such as HE 12 and HE 41 may also be excited by light propagating along the nonadiabatic downtaper. Among all the higher-order modes, LP 11 will be the most strongly excited, since the fiber sags during pulling [39]; this agrees with our beat length measurements shown in Table 1. Previously, it was shown that [6] by choosing a particular ratio of the resonator size to the diameter of the tapered fiber, only the HE 11 and LP 11 modes can significantly interact with the WGMs of a microresonator, and therefore, any weak excitation of other higher-order modes can be neglected.…”
Section: Fabrication Modeling and Testing Of Asymmetric Tapered Fibersupporting
confidence: 89%
“…It is worth noting that in addition to the HE 11 and LP 11 modes, other higher-order modes such as HE 12 and HE 41 may also be excited by light propagating along the nonadiabatic downtaper. Among all the higher-order modes, LP 11 will be the most strongly excited, since the fiber sags during pulling [39]; this agrees with our beat length measurements shown in Table 1. Previously, it was shown that [6] by choosing a particular ratio of the resonator size to the diameter of the tapered fiber, only the HE 11 and LP 11 modes can significantly interact with the WGMs of a microresonator, and therefore, any weak excitation of other higher-order modes can be neglected.…”
Section: Fabrication Modeling and Testing Of Asymmetric Tapered Fibersupporting
confidence: 89%
“…1(b), one of which is responsible for the higher-order modes (HOMs) excitation (the left taper), while the other taper acts as a phase-matching component to form interferometry between the HOMs and the fundamental mode. Based on the taper's geometry and the RI contrast of the SMF, the modes' excitation order and power evolution can be calculated using the CMT [11], [17]- [20]. The power evolution calculation provides us with a set of linearly polarized (LP) modes {Ψ ν }, their Effective Refractive Indices (ERIs) {n ν }, and complex amplitudes {A ν } along each taper; ν is the mode index.…”
Section: Theorymentioning
confidence: 99%
“…Amongst all, the latter in the form of a Double-Taper Mach-Zehnder Interferometer (DTMZI) shows more promise as it can be fabricated quickly with the essential tools in hand, namely single-mode fiber (SMF) and fusion splicer [8]. Moreover, abrupt taper's modeling and its fabrication imperfections have been thoroughly investigated via recent works [9]- [11]. The application of measuring axial strain has been studied on DTMZI, and their modal behaviour has been thoroughly studied [12], [13].…”
Section: Introductionmentioning
confidence: 99%
“…During the bending process of the LPFG, the mode field distribution of the core fundamental and cladding modes change, subsequently changing the coupling coefficient between them. In recent years, many optical fibre curvature sensors based on different optical devices have been proposed, such as LPFG [10][11][12][13][14][15], FBG [16,17], multi-core fibre [18,19], photonic crystal fibre [20,21] and fibre tapers [22] etc. In terms of curvature measurement of LPFG, Zhang et al [10] designed an arch-shaped LPFG that detects vector bending in two orthogonal directions.…”
Section: Introductionmentioning
confidence: 99%