Deuterium treatment of low water peak fiber

doi:10.1007/s12200-009-0039-3

Front Optoelec Chin

2009, Vol. 2

Issue (2) : 178-181 https://doi.org/10.1007/s12200-009-0039-3

RESEARCH ARTICLE

Deuterium treatment of low water peak fiber

Xinwei QIAN(

), Deming LIU, Feng TU

College of Optoelectronic Science and Engineering, Huazhong University of Science and Technology, Wuhan 430074, China

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Abstract

The deuterium (D₂) treatment of low water peak single-mode fiber (LWP-SMF) after drawing has been investigated. The D₂ treatment time and concentration have important effect on fiber’s properties after D₂ treatment. The insufficient treatment of D₂ cannot ensure fiber resistant to hydrogen aging, whereas excessive treatment of D₂ will result in excess loss on fiber at 1383 nm. The optimization on viscosity match between the core and the cladding is helpful on problem solving of excess loss after the D₂ treatment. However, by designing proper time and D₂ concentration in the D₂ treatment process, it can produce fiber with good hydrogen aging resistance and low excess loss and lower the cost of the D₂ treatment process.

Keywords deuterium (D₂) treatment time concentration excess loss low water peak (LWP) fiber

Corresponding Author(s): QIAN Xinwei,Email:qianxinwei@yofc.com

Issue Date: 05 June 2009

Cite this article:

Xinwei QIAN,Deming LIU,Feng TU. Deuterium treatment of low water peak fiber[J]. Front Optoelec Chin, 2009, 2(2): 178-181.

URL:

https://academic.hep.com.cn/foe/EN/10.1007/s12200-009-0039-3
https://academic.hep.com.cn/foe/EN/Y2009/V2/I2/178

Fig.1 Schematic structure of D treatment system

Fig.2 HIL of fibers samples. (a) HIL at 1383 nm; (b) HIL at 1530 nm

Fig.3 Excess loss at 1383 nm of fiber after D treatment

Fig.4 RI and viscosity profile of optimized SMF. (a) RI profile; (b) viscosity profile

1	Marshall A, Irven J, Pitt N J. Hydrogen and deuterium gas-in-glass effects in single-mode optical fibers. IEE proceedings Part J Optoelectronics , 1985, 132(3): 172–176
2	Stone J. Reduction of OH absorption in optical fibers by OH→OD isotope exchange. Industrial and Engineering Chemistry Product Research and Development , 1986, 25(4): 609–621
3	Matthijsse P, Simons D R, Zhang S Q, Luo J, Vydra J, Fabian H. Towards the low limits of 1383 nm loss in PCVD enabled single mode fibre production. In: Proceedings of Optical Fiber Communication Conference 2004 . 2004, 12–15
4	Tomita A, Lemaire P J. Hydrogen-induced loss increases in germanium-doped single-mode optical fibers: long-term predictions. Electronics Letters , 1985, 21(2): 71–72
5	Stone J. Interactions of hydrogen and deuterium with silica optical fibers: a review. Journal of Lightwave Technology , 1987, 5(5): 712–733

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