Laser and photoluminescence spectra of InGaAs–GaAs strained-layer superlattices

1989 ◽  
Vol 67 (4) ◽  
pp. 394-399 ◽  
Author(s):  
N. E. J. Hunt ◽  
P. E. Jessop ◽  
B. K. Garside ◽  
R. L. S. Devine

Photoluminescence (PL) and laser emission from optically excited InxGa1−xAs–GaAs strained-layer superlattices (SLS) grown by molecular-beam epitaxy have been examined. In low-intensity PL, a single, narrow (≈5 nm FWHM) emission peak was observed, corresponding to the n = 1 electron to heavy-hole transition. This feature, as well as a series of higher energy transitions, was also observed in absorption and photoreflectance spectra. High-intensity PL, using a pulsed nitrogen laser for excitation, yielded an additional peak, several millielectronvolts lower in energy than the dominant low-power PL feature. Optical-gain measurements were performed using the variable stripe-length method. The stimulated emission emerging from the single cleaved end was shifted to the long-wavelength side of the low-power PL peak, and in the case of the narrower well samples, the emission consisted of two peaks separated by about 8 meV. Lasing at these gain positions was observed when ≈400 μm long chips were prepared and their lengths were pumped with a stripe of nitrogen laser light. The observed gain spectrum has been attributed to a combination of a free-carrier-induced bandgap shift and self-absorption by unpumped material deeper within the SLS waveguide.

1992 ◽  
Vol 61 (18) ◽  
pp. 2190-2192 ◽  
Author(s):  
Yoichi Yamada ◽  
Yasuaki Masumoto ◽  
John T. Mullins ◽  
Tsunemasa Taguchi

Author(s):  
J.M. Brown ◽  
M.E. Mochel ◽  
N. Holonyak ◽  
M.D. Camras ◽  
M.J. Ludowise ◽  
...  

The epitaxial growth of mismatched or strained III-V layers was shown to be viable as early as 1960. Osbourn et al suggested that strained layer GaP-GaAs1-xPx superlattices grown by organo-metal1ic vapor phase epitaxy (OMVPE) could be used to fold the Brillouin zone and make indirect-crystal direct. More recently, it has been shown that a strained-layer superlattice can be grown free enough of defects at heterointerfaces to make possible stimulated emission. This has been demonstrated on OMVPE GaAs1-xPx-GaAs (x=0.25) and GaAs-InxGa1-xAs (x=0.2) strained layer superlattices which have been operatedas photopuraped continuous (cw) 300K lasers but which at high excitation levels (> 103Acm-2) prove to be unstable. This paper presents the results of an electron microscope study of the defects produced in a GaAs-InxGa1-xAs strained superlattice as a result of high excitation levels of operation.


1990 ◽  
Vol 216 ◽  
Author(s):  
Steven R. Kurtz

ABSTRACTAn overview is provided of long wavelength, photovoltaic detectors constructed with type II (also known as “staggered”), III-V superlattices. Specifically, the electronic properties of InAsSb strained-layer superlattices and prototype detectors utilizing these structures are described.


1984 ◽  
Vol 37 ◽  
Author(s):  
N. G. Anderson ◽  
W. D. Laidig ◽  
G. Lee ◽  
Y. Lo ◽  
M. Ozturk

AbstractThe low-temperature (20K) photoluminescence of InxGa1-xAs and InxGal-xAs - GaAs strained-layer superlattices (SLS's) grown by molecular beam epitaxy (MBE) is investigated. Data are presented for thick (bulk) epitaxial layers grown directly on GaAs and for relatively-thin (˜600Å) InxGa1-xAs layers under biaxial compression. Data are also presented for two series of SLS's. In the two series of SLS's, the InxGa1-xAs layer thickness (Lz) is held constant while only the GaAs layer thickness (LB) is varied. The photoluminescence (PL) spectra of the crystals are useful in analyzing the effects of biaxial strain, carrier confinement, and barrier layer thicknesses in SLS's. Results are compared with calculations based upon a modified Kronig-Penney model which incorporates the appropriate deformation potentials for SLS analysis. This type of analysis, in agreement with experimental data, suggests that the electron-to-light-hole transition can be lower in energy than the electron-to-heavy-hole transition in SLS's, depending upon layer thickness and crystal composition.


2012 ◽  
Vol 101 (17) ◽  
pp. 171105 ◽  
Author(s):  
H. J. Haugan ◽  
G. J. Brown ◽  
S. Elhamri ◽  
W. C. Mitchel ◽  
K. Mahalingam ◽  
...  

1987 ◽  
Vol 48 (C5) ◽  
pp. C5-321-C5-327 ◽  
Author(s):  
H. BRUGGER ◽  
G. ABSTREITER

2007 ◽  
Vol 91 (4) ◽  
pp. 043514 ◽  
Author(s):  
J. B. Rodriguez ◽  
E. Plis ◽  
G. Bishop ◽  
Y. D. Sharma ◽  
H. Kim ◽  
...  

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