Paper
9 July 2001 Modeling of optically pumped type-II lasers
Yao-Ming Mu, Han Q. Le, Shin Shem Pei
Author Affiliations +
Abstract
The electronic structures of (InAs)m/(GaSb)n short- period superlattices are investigated by the empirical pseudo potential method and multiband kp envelope function approximation with the same underlying bulk band structures. The calculated result are compared to each other and with experiment. Generally, the results of the empirical pseudo potential method are in better agreement with the experimental measurement. The superlattice active region of an optically-pumped type-II laser are investigated by the empirical pseudo potential method. The calculated result predict that its lasing wavelength is about 3.5 micrometers at 80K and internal losses due to intervalence absorption have been suppressed.
© (2001) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only.
Yao-Ming Mu, Han Q. Le, and Shin Shem Pei "Modeling of optically pumped type-II lasers", Proc. SPIE 4283, Physics and Simulation of Optoelectronic Devices IX, (9 July 2001); https://doi.org/10.1117/12.432563
Lens.org Logo
CITATIONS
Cited by 2 scholarly publications.
Advertisement
Advertisement
RIGHTS & PERMISSIONS
Get copyright permission  Get copyright permission on Copyright Marketplace
KEYWORDS
Superlattices

Laser optics

Heterojunctions

Absorption

Interfaces

Active optics

Gallium antimonide

RELATED CONTENT

Novel narrow-gap semiconductor systems
Proceedings of SPIE (March 01 1991)
W structured type II superlattice based long and very...
Proceedings of SPIE (March 25 2005)
Modeling of mid-IR type-II interband cascade lasers
Proceedings of SPIE (July 14 2000)
The role of InAs thickness on the material properties of...
Proceedings of SPIE (September 16 2011)
Short-period superlattices: is thinner better?
Proceedings of SPIE (February 28 2006)
Interfaces as design tools for short period InAs GaSb type...
Proceedings of SPIE (September 29 2005)

Back to Top