Birefringence properties of anti-resonant octagonal-core and nodeless hollow-core fibers

Stanislav O. Leonov; Elizaveta A. Yelistratova; Vladimir V. Demidov; Andrey D. Pryamikov

doi:10.1364/AO.392175

Applied Optics
Vol. 59,
Issue 16,
pp. 5013-5019
(2020)
•https://doi.org/10.1364/AO.392175

Birefringence properties of anti-resonant octagonal-core and nodeless hollow-core fibers

Stanislav O. Leonov, Elizaveta A. Yelistratova, Vladimir V. Demidov, and Andrey D. Pryamikov

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Stanislav O. Leonov, Elizaveta A. Yelistratova, Vladimir V. Demidov, and Andrey D. Pryamikov, "Birefringence properties of anti-resonant octagonal-core and nodeless hollow-core fibers," Appl. Opt. 59, 5013-5019 (2020)

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- Fiber Optics, Fiber Sensors, and Optical Communications
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About this Article
History
- Original Manuscript: March 17, 2020
- Revised Manuscript: May 5, 2020
- Manuscript Accepted: May 7, 2020
- Published: June 1, 2020

Abstract

We present experimental results of birefringence property measurements for two types of negative curvature anti-resonant hollow-core fibers (AR-HCFs). Both AR-HCFs have a core of 50 µm in diameter, providing an effective area of the fundamental guided mode larger than $1000\;\unicode{x00B5}{\rm m}^2$. Measurements were carried out at wavelengths of 2.25, 2.35, and 2.45 µm. The obtained results demonstrate that both fiber types have birefringence axes that do not correspond to core symmetry axes. The proposed technique for the birefringence axes orientation measurement could be applied to other kinds of HCFs at various wavelengths.

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Wavelength (µm)	Octagonal-Core		Nodeless
Wavelength (µm)	$θ_{l} (^{\circ})$	$\frac{τ_{min}}{τ_{max}}$	$θ_{l} (^{\circ})$	$\frac{τ_{min}}{τ_{max}}$
2.25	$22.3 \pm 6.9$	$0.74 \pm 0.04$	$149.1 \pm 34.3$	$0.96 \pm 0.03$
2.35	$25.3 \pm 1.7$	$0.56 \pm 0.02$	$100.5 \pm 18.8$	$0.97 \pm 0.01$
2.45	$37.4 \pm 1.8$	$0.09 \pm 0.03$	$76.6 \pm 7.4$	$0.70 \pm 0.04$

Wavelength (µm)	Octagonal-Core				Nodeless
Wavelength (µm)	$θ_{b} (^{\circ})$	$δ (^{\circ})$	$Δ n$	$τ_{r}$	$θ_{b} (^{\circ})$	$δ (^{\circ})$	$Δ n$	$τ_{r}$
2.25	$52.9 \pm 2.3$	$36.9 \pm 3.2$	$7 \cdot 10^{- 7}$	$0.87 \pm 0.12$	$22.9 \pm 3.6$	$40.7 \pm 5.5$	$8 \cdot 10^{- 7}$	$1.01 \pm 0.06$
2.35	$54.3 \pm 2.2$	$59.4 \pm 4.9$	$1 \cdot 10^{- 7}$	$0.74 \pm 0.11$	$16.5 \pm 3.1$	$37.4 \pm 4.6$	$8 \cdot 10^{- 7}$	$1.02 \pm 0.01$
2.45	$52.5 \pm 5.8$	$36.3 \pm 6.9$	$8 \cdot 10^{- 7}$	$0.17 \pm 0.11$	$21.3 \pm 4.9$	$75.1 \pm 14.6$	$2 \cdot 10^{- 6}$	$1.13 \pm 0.18$

Wavelength (µm)	Octagonal-Core		Nodeless
Wavelength (µm)	$θ_{l} (^{\circ})$	$\frac{τ_{min}}{τ_{max}}$	$θ_{l} (^{\circ})$	$\frac{τ_{min}}{τ_{max}}$
2.25	$22.3 \pm 6.9$	$0.74 \pm 0.04$	$149.1 \pm 34.3$	$0.96 \pm 0.03$
2.35	$25.3 \pm 1.7$	$0.56 \pm 0.02$	$100.5 \pm 18.8$	$0.97 \pm 0.01$
2.45	$37.4 \pm 1.8$	$0.09 \pm 0.03$	$76.6 \pm 7.4$	$0.70 \pm 0.04$

Wavelength (µm)	Octagonal-Core				Nodeless
Wavelength (µm)	$θ_{b} (^{\circ})$	$δ (^{\circ})$	$Δ n$	$τ_{r}$	$θ_{b} (^{\circ})$	$δ (^{\circ})$	$Δ n$	$τ_{r}$
2.25	$52.9 \pm 2.3$	$36.9 \pm 3.2$	$7 \cdot 10^{- 7}$	$0.87 \pm 0.12$	$22.9 \pm 3.6$	$40.7 \pm 5.5$	$8 \cdot 10^{- 7}$	$1.01 \pm 0.06$
2.35	$54.3 \pm 2.2$	$59.4 \pm 4.9$	$1 \cdot 10^{- 7}$	$0.74 \pm 0.11$	$16.5 \pm 3.1$	$37.4 \pm 4.6$	$8 \cdot 10^{- 7}$	$1.02 \pm 0.01$
2.45	$52.5 \pm 5.8$	$36.3 \pm 6.9$	$8 \cdot 10^{- 7}$	$0.17 \pm 0.11$	$21.3 \pm 4.9$	$75.1 \pm 14.6$	$2 \cdot 10^{- 6}$	$1.13 \pm 0.18$

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Applied Optics