Tunable fiber soliton laser

Guofu Chen; Wei Hu; Dongfeng Liu; Xianhua Wang; Xun Hou

doi:10.1117/12.273443

Tunable fiber soliton laser

Guofu Chen
, Wei Hu
, Dongfeng Liu
, Xianhua Wang
, Xun Hou

Faculty of Electronic and Information Engineering

CAS - Xi'an Institute of Optics and Precision Mechanics

Research output: Contribution to journal › Conference article › peer-review

Abstract

This paper describes a tunable fiber soliton laser. This laser is configured as a ring with a silica optical fiber gain medium.A length of 300m conventional fiber provides the negative group velocity dispersion, self-phase modulation and Raman gain effect. The time-dispersion tuning technology is used for wavelength selection, because the Raman gain of silica fiber has a wide spectrum. The different wavelengths have different optical lengths, when they propagate in a optical fiber. We use an active modelocking Nd:YLF Laser which has wavelength 1.313 mn with pulse width of 70ps for pumping source and silica optical fiber of 300m for gain medium and group velocity dispersion compensator.The pulse width(FWHM)of 195fs has been got, the laser wavelength is 1.395 \i m and tunable region of 47nm near 1.397 |i m.

Original language	English
Pages (from-to)	502-507
Number of pages	6
Journal	Proceedings of SPIE - The International Society for Optical Engineering
Volume	2869
DOIs	https://doi.org/10.1117/12.273443
State	Published - 28 May 1997
Event	22nd International Congress on High-Speed Photography and Photonics 1996 - Santa Fe, United States Duration: 27 Oct 1996 → 1 Nov 1996

Keywords

Femtosecond
Fiber laser
Synchronous pumping
Tunable

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10.1117/12.273443

Cite this

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title = "Tunable fiber soliton laser",

abstract = "This paper describes a tunable fiber soliton laser. This laser is configured as a ring with a silica optical fiber gain medium.A length of 300m conventional fiber provides the negative group velocity dispersion, self-phase modulation and Raman gain effect. The time-dispersion tuning technology is used for wavelength selection, because the Raman gain of silica fiber has a wide spectrum. The different wavelengths have different optical lengths, when they propagate in a optical fiber. We use an active modelocking Nd:YLF Laser which has wavelength 1.313 mn with pulse width of 70ps for pumping source and silica optical fiber of 300m for gain medium and group velocity dispersion compensator.The pulse width(FWHM)of 195fs has been got, the laser wavelength is 1.395 \textbackslash{}i m and tunable region of 47nm near 1.397 |i m.",

keywords = "Femtosecond, Fiber laser, Synchronous pumping, Tunable",

author = "Guofu Chen and Wei Hu and Dongfeng Liu and Xianhua Wang and Xun Hou",

note = "Publisher Copyright: {\textcopyright} 1997 SPIE. All rights reserved.; 22nd International Congress on High-Speed Photography and Photonics 1996 ; Conference date: 27-10-1996 Through 01-11-1996",

year = "1997",

month = may,

day = "28",

doi = "10.1117/12.273443",

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TY - JOUR

T1 - Tunable fiber soliton laser

AU - Chen, Guofu

AU - Hu, Wei

AU - Liu, Dongfeng

AU - Wang, Xianhua

AU - Hou, Xun

PY - 1997/5/28

Y1 - 1997/5/28

N2 - This paper describes a tunable fiber soliton laser. This laser is configured as a ring with a silica optical fiber gain medium.A length of 300m conventional fiber provides the negative group velocity dispersion, self-phase modulation and Raman gain effect. The time-dispersion tuning technology is used for wavelength selection, because the Raman gain of silica fiber has a wide spectrum. The different wavelengths have different optical lengths, when they propagate in a optical fiber. We use an active modelocking Nd:YLF Laser which has wavelength 1.313 mn with pulse width of 70ps for pumping source and silica optical fiber of 300m for gain medium and group velocity dispersion compensator.The pulse width(FWHM)of 195fs has been got, the laser wavelength is 1.395 \i m and tunable region of 47nm near 1.397 |i m.

AB - This paper describes a tunable fiber soliton laser. This laser is configured as a ring with a silica optical fiber gain medium.A length of 300m conventional fiber provides the negative group velocity dispersion, self-phase modulation and Raman gain effect. The time-dispersion tuning technology is used for wavelength selection, because the Raman gain of silica fiber has a wide spectrum. The different wavelengths have different optical lengths, when they propagate in a optical fiber. We use an active modelocking Nd:YLF Laser which has wavelength 1.313 mn with pulse width of 70ps for pumping source and silica optical fiber of 300m for gain medium and group velocity dispersion compensator.The pulse width(FWHM)of 195fs has been got, the laser wavelength is 1.395 \i m and tunable region of 47nm near 1.397 |i m.

KW - Femtosecond

KW - Fiber laser

KW - Synchronous pumping

KW - Tunable

UR - https://www.scopus.com/pages/publications/85077783088

U2 - 10.1117/12.273443

DO - 10.1117/12.273443

M3 - 会议文章

AN - SCOPUS:85077783088

SN - 0277-786X

VL - 2869

SP - 502

EP - 507

JO - Proceedings of SPIE - The International Society for Optical Engineering

JF - Proceedings of SPIE - The International Society for Optical Engineering

T2 - 22nd International Congress on High-Speed Photography and Photonics 1996

Y2 - 27 October 1996 through 1 November 1996

ER -

Tunable fiber soliton laser

Abstract

Keywords

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