2003
DOI: 10.1016/s1631-0705(03)00098-7
|View full text |Cite
|
Sign up to set email alerts
|

GaSb-based mid-infrared 2–5 μm laser diodes

Abstract: Laser diodes emitting at room temperature in continuous wave regime (CW) in the mid-infrared (2-5 µm spectral domain) are needed for applications such as high sensitivity gas analysis by tunable diode laser absorption spectroscopy (TDLAS) and environmental monitoring. Such semiconductor devices do not exist today, with the exception of type-I GaInAsSb/AlGaAsSb quantum well laser diodes which show excellent room temperature performance, but only in the 2.0-2.6 µm wavelength range. Beyond 2.6 µm, type-II GaInAsS… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

3
41
0
2

Year Published

2006
2006
2017
2017

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 77 publications
(47 citation statements)
references
References 94 publications
3
41
0
2
Order By: Relevance
“…Both COMSOL simulations and 6 × 6 k.p calculations [16] confirm that the ground heavy hole (GHH) state was the only confined energy state within QDs of base radius 1.25-3 nm. For both pure InSb QDs (~1.25 nm) and larger InAs0.6Sb0.4 QDs (~3 nm), the electron-hole wave function overlap lies within the range 35%-40% (using both simulation methods), which is lower than in type I QDs and W-structures [18,19]. However, due to the high QD density, an exceptionally high material gain of ~20 × 10 4 cm −1 can be estimated for our type II QD, which is in the same range as for type I QDs [13].…”
Section: Gain From Insb Qdsmentioning
confidence: 87%
“…Both COMSOL simulations and 6 × 6 k.p calculations [16] confirm that the ground heavy hole (GHH) state was the only confined energy state within QDs of base radius 1.25-3 nm. For both pure InSb QDs (~1.25 nm) and larger InAs0.6Sb0.4 QDs (~3 nm), the electron-hole wave function overlap lies within the range 35%-40% (using both simulation methods), which is lower than in type I QDs and W-structures [18,19]. However, due to the high QD density, an exceptionally high material gain of ~20 × 10 4 cm −1 can be estimated for our type II QD, which is in the same range as for type I QDs [13].…”
Section: Gain From Insb Qdsmentioning
confidence: 87%
“…They have used various structures such as photodiodes (PD), light source/ detector (LED/PD) pair. Material systems have used to grow such predominantly based on type-II InAs/GaSb superlattice (T2SL), mercury cadmium telluride (MCT) and extended indium gallium arsenide (InGaAs) and quaternary InGaAsSb materials [3]. Among them, the InGaAsSb material system have been developed for IR-LED and PD.…”
Section: Introductionmentioning
confidence: 99%
“…The epitaxial technology of antimonides on GaSb finds application in several electronic and optoelectronic devices such as lasers, detectors or photo− and thermo− voltaic cells [1][2][3][4][5][6][7][8][9][10][11][12][13][14]. While for other III−V materials, two main epitaxial techniques − MBE and MOCVD − usually enable the pro− duction of the layers with comparable quality, in the case of antimonides on GaSb, MBE currently yields better material than MOCVD.…”
Section: Introductionmentioning
confidence: 99%
“…While for other III−V materials, two main epitaxial techniques − MBE and MOCVD − usually enable the pro− duction of the layers with comparable quality, in the case of antimonides on GaSb, MBE currently yields better material than MOCVD. This is of special concern for the realisation of lasers [1][2][3][4][5][6][7][8], where the deficiency of stable antimony hydride precursor contributes to high oxygen and carbon contamination of aluminium containing layers [9]. On the other hand, MOCVD presents benefits such as lower pro− duction cost, which stimulates research in this field.…”
Section: Introductionmentioning
confidence: 99%