Literature DB >> 22410883

High-spectral-flatness mid-infrared supercontinuum generated from a Tm-doped fiber amplifier.

Jihong Geng1, Qing Wang, Shibin Jiang.   

Abstract

Broadband mid-infrared supercontinuum pulses were generated directly from a short piece of active fiber in a single-mode Tm-doped fiber amplifier. The broadband mid-infrared pulses have an extremely high spectral flatness with ~600 nm FWHM bandwidth (from 1.9 μm to 2.5 μm), >15 kW peak power, and >20 GW/cm(2) laser peak intensity. This new approach exhibits a significantly different physical mechanism from other supercontinuum generation demonstrations in the literature, in which usually a piece of passive fiber was used for nonlinear spectral broadening. The physical mechanism for the broadband mid-infrared supercontinuum generation in this approach has been attributed to a combined effect of two superradiative processes of Tm(3+) ions (i.e., the (3)F(4)-(3)H(6) transition covering the 1.8~2.1  μm spectral region and the (3)H(4)-(3)H(5) transition covering the 2.2~2.5  μm spectral region), and also nonlinear optical processes as well in the Tm-doped gain fiber. The spectra of the mid-infrared supercontinuum pulses were further broadened in a 2 m chalcogenide fiber with 20 dB bandwidth ~1100 nm and a 3 m fluoride fiber with 20 dB bandwidth ~2600 nm.
© 2012 Optical Society of America

Entities:  

Year:  2012        PMID: 22410883     DOI: 10.1364/AO.51.000834

Source DB:  PubMed          Journal:  Appl Opt        ISSN: 1559-128X            Impact factor:   1.980


  2 in total

1.  Super-flat supercontinuum generation from a Tm-doped fiber amplifier.

Authors:  Mengmeng Tao; Ting Yu; Zhenbao Wang; Hongwei Chen; Yanlong Shen; Guobin Feng; Xisheng Ye
Journal:  Sci Rep       Date:  2016-03-29       Impact factor: 4.379

2.  Dual-band Tm3+-doped tellurite fiber amplifier and laser at 1.9 μm and 2.3 μm.

Authors:  S V Muravyev; E A Anashkina; A V Andrianov; V V Dorofeev; S E Motorin; M Y Koptev; A V Kim
Journal:  Sci Rep       Date:  2018-11-01       Impact factor: 4.379

  2 in total

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