2002
DOI: 10.1109/lpt.2002.1021965
|View full text |Cite
|
Sign up to set email alerts
|

Efficient direct locking of colliding pulse mode-locked lasers on semi-insulating substrate at 1.5 μm

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
2
0

Year Published

2004
2004
2016
2016

Publication Types

Select...
3
2

Relationship

0
5

Authors

Journals

citations
Cited by 14 publications
(2 citation statements)
references
References 3 publications
0
2
0
Order By: Relevance
“…Colliding Pulse Mode Locked Lasers (CPM) offer many advantages compared to other mode locked lasers providing relatively stable and better pulse-shaped mode-locking operation [1,2,4]. In this paper, we report for the first time the electrical subharmonic hybrid mode-locking (SHML) of a 3000 ,um buried heterostructure (BH) CPM laser fabricated through a single step MOVPE regrowth process with nearly transform-limited output.…”
Section: Introductionmentioning
confidence: 99%
“…Colliding Pulse Mode Locked Lasers (CPM) offer many advantages compared to other mode locked lasers providing relatively stable and better pulse-shaped mode-locking operation [1,2,4]. In this paper, we report for the first time the electrical subharmonic hybrid mode-locking (SHML) of a 3000 ,um buried heterostructure (BH) CPM laser fabricated through a single step MOVPE regrowth process with nearly transform-limited output.…”
Section: Introductionmentioning
confidence: 99%
“…[1−4] Compared with traditional Fabry-Perot two-section type mode-locked configurations, of which typical schemes incorporate a gain section and a saturable absorber (SA) that is integrated on a single substrate sharing the same multiple quantum well active region, [5−8] colliding pulse mode-locked (CPM) lasers place the SA section at the center of the laser cavity, taking advantage of the collision of two counter-propagating pulses in the SA section, which results in an absorption grating, leading to an enhancement of the saturable absorption and therefore more effective pulse shortening. [9−12] CPM lasers with 40-GHz repetition rate have been realized earlier in bulk [13] and multi-quantum well InGaAsP lasers [14] with picosecond pulses obtained. However, both the structures employed an all-active configuration, which would introduce potentially too much quantum noise resulting from amplified spontaneous emission (ASE) of the gain section, [15] leading to broad rf 3-dB line widths of several hundreds of kilohertz, deteriorating the device performance in pragmatic applications.…”
mentioning
confidence: 99%