1997
DOI: 10.1049/el:19970585
|View full text |Cite
|
Sign up to set email alerts
|

Erbium-doped tellurite glass fibre laser and amplifier

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3

Citation Types

0
109
0
7

Year Published

2001
2001
2016
2016

Publication Types

Select...
5
5

Relationship

1
9

Authors

Journals

citations
Cited by 285 publications
(124 citation statements)
references
References 9 publications
0
109
0
7
Order By: Relevance
“…Lasing in a tellurite fiber was first reported in 1994 at 1.061 mi na nN d 3+ -doped fiber [4] and again in 1997 at 1.560 mi na nE r 3+ -doped fiber [5]. Both of these tellurite fiber lasers were of a single-mode design constructed using a 12%-12% cavity from Fresnel reflections from the bare fiber ends.…”
mentioning
confidence: 99%
“…Lasing in a tellurite fiber was first reported in 1994 at 1.061 mi na nN d 3+ -doped fiber [4] and again in 1997 at 1.560 mi na nE r 3+ -doped fiber [5]. Both of these tellurite fiber lasers were of a single-mode design constructed using a 12%-12% cavity from Fresnel reflections from the bare fiber ends.…”
mentioning
confidence: 99%
“…Stimulated Brillouin Scattering and Stimulated Raman Scattering) limiting the achievable peak power, which are exacerbated by the narrow linewidth output requirement of gas spectroscopy. Moreover due to the higher emission cross section offered by tellurite glasses with respect to silicates [4,5], there is the potential to make a more compact gain-module for the power amplifier stage in a MOPA system, like the one being developed for the ASCENDS space mission [1]. To date in our samples we have measured gains of 2 dBcm -1 at the 1535 nm peak and 0.7 dBcm -1 around 1575 nm the key wavelength of interest.…”
Section: Introductionmentioning
confidence: 98%
“…Stimulated Brillouin Scattering and Stimulated Raman Scattering) can be mitigated and enable higher peak powers despite the very narrow linewidth requirement for gas spectroscopy. Moreover due to the higher emission cross section offered by these glasses with respect to silicates [4,5], there is the potential to make a more compact gain-module for the power amplifier stage in a MOPA system. To date in our samples we have measured, with in-band pumping at approximately the saturation irradiance for the glasses, gains in excess of 2 dBcm -1 at the 1535 nm peak and 0.7 dBcm -1 around 1572 nm the key wavelength of interest.…”
Section: Introductionmentioning
confidence: 99%