2019
DOI: 10.1364/optica.6.001071
|View full text |Cite
|
Sign up to set email alerts
|

Large linewidth reduction in semiconductor lasers based on atom-like gain material

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
21
1

Year Published

2020
2020
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 46 publications
(22 citation statements)
references
References 32 publications
0
21
1
Order By: Relevance
“…One important aspect of QD lasers is the small -factor that contributes to significant reductions in the laser linewidth [36] The state-of-the-art 1550 nm InAs/InP QD DFB lasers can achieve linewidths of less than 50 kHz by applying a very low reflectivity antireflection coating (AR) on both facets. [37] For 1300 nm InAs/GaAs QD DFB lasers, the first excited state can be easily populated when increasing the bias.…”
Section: Measurement and Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…One important aspect of QD lasers is the small -factor that contributes to significant reductions in the laser linewidth [36] The state-of-the-art 1550 nm InAs/InP QD DFB lasers can achieve linewidths of less than 50 kHz by applying a very low reflectivity antireflection coating (AR) on both facets. [37] For 1300 nm InAs/GaAs QD DFB lasers, the first excited state can be easily populated when increasing the bias.…”
Section: Measurement and Analysismentioning
confidence: 99%
“…[37] For 1300 nm InAs/GaAs QD DFB lasers, the first excited state can be easily populated when increasing the bias. [36] This leads to an asymmetric gain spectrum with increased -factor, and consequently much larger linewidths. However, with highly uniform dot size distributions, the -factor of our InAs/GaAs QD lasers can be as low as 0.13.…”
Section: Measurement and Analysismentioning
confidence: 99%
“…As a complementary derivation to the one followed above, focusing on the RRM as a light storage element, one can also observe that the phase noise to intensity noise conversion seen here arises from the dispersion inherent to the resonator transfer function, similarly to phase to amplitude noise conversion during propagation over long segments of dispersive fiber [23]. This dispersion is zeroed on resonance due to the symmetricity of the transfer function, similarly to the zeroing of the linewidth broadening factor in lasers (also corresponding to phase noise to intensity noise conversion) when using ideal atomic like gain media with a symmetric gain spectrum [24].…”
Section: #$mentioning
confidence: 63%
“…On one hand, InAs QDs grown on GaAs substrate are ideal for a wide range of short-reach communications (1260–1360 nm) that is to say for integrated technologies, sensing, compact laser-based radars, and high performance computing 15 , 20 , 21 . On the other hand, InAs QDs grown on InP substrates are more prone to long-reach communications (1530–1565 nm) namely for access, metro and core optical networks 22 , 23 . High performance InAs/InP QD lasers can be achieved, however, compared with InAs/GaAs, the formation of “true” InAs QDs on InP is more challenging since the lattice mismatch in InAs/InP (3%) is smaller than that in InAs/GaAs (7%) 21 .…”
Section: Introductionmentioning
confidence: 99%
“…It is noted that every AR/HR laser may also exhibit different spectral linewidth characteristics and random facet phase effects which can be problematic for practical and industrial applications. Recently, a narrow intrinsic linewidth of 30 kHz has also been obtained in a high performance QD DFB laser 23 . Fig.…”
Section: Introductionmentioning
confidence: 99%