Low pressure MOCVD growth of buried heterostructure laser wafers using high quality semi-insulating InP

1992 ◽  
Vol 21 (2) ◽  
pp. 165-171 ◽  
Author(s):  
D. G. Knight ◽  
B. Emmerstorfer ◽  
G. Pakulski ◽  
C. Larocque ◽  
A. J. Springthorpe
1988 ◽  
Vol 126 ◽  
Author(s):  
M. Razeghi ◽  
M. Defour ◽  
F. Omnes ◽  
J. Nagle ◽  
P. Maurel ◽  
...  

ABSTRACTHigh quality GaAs and InP have been grown on silicon substrates, using low pressure metalorganic chemical vapor deposition technique. The growth temperature is 550°C and the growth rate 100 A/min.Photoluminescence, X-ray diffraction and electrochemical profiling verified the high quality of these layers. The use of superlattices as buffer layers, (GaAs/GaInP) in the case of GaAs/Si and (GaInAsP/InP) in the case of InP/Si, decreased the amount of misfit dislocations in the epitaxial layer. Carrier concentrations as low as 5.1015 cm−3 have been measured by electrochemical profiling.


1988 ◽  
Vol 116 ◽  
Author(s):  
M. Razeghi ◽  
M. Defour ◽  
F. Omnes ◽  
J. Nagle ◽  
P. Maurel ◽  
...  

AbstractHigh quality GaAs and InP have been grown on silicon substrates, using low pressure metalorganic chemical vapor deposition technique. The growth temperature is 550ºC andthe growth rate 100 A/min.Photoluminescence, X-ray diffraction and electrochemical profiling verified the high quality of these layers. The use of superlattices as buffer layers, (GaAs/GaInP) in the case of GaAs/Si and (GalnAsP/InP) in the case of InP/Si, decreased the amount of misfit dislocations in the epitaxial layer. Carrier concentrations as low as 5.1015 cm-3 have been measured by electrochemical profiling.


1993 ◽  
Author(s):  
Naresh Chand ◽  
Niloy K. Dutta ◽  
Sung-Nee G. Chu ◽  
Alexei V. Syrbou ◽  
Alexandru Z. Mereutza ◽  
...  

1990 ◽  
Vol 216 ◽  
Author(s):  
B.T. Cunningham ◽  
R.P. Schneider ◽  
R.M. Biefeld

ABSTRACTLow pressure (200 Torr) metalorganic chemical vapor deposition (MOCVD) of InSb has been examined through variation of the Column III (TMIn) and Column V (TMSb or TESb) precursor partial pressures. The use of lower growth pressure significantly enhanced the range of allowable Column III and Column V partial pressures in which specular morphology InSb could be obtained without the formation of In droplets or Sb crystals. In addition, a 70% improvement in the average hole mobility was obtained, compared to InSb grown in the same reactor at atmospheric pressure. SIMS analysis revealed that Si at the substrate/epitaxial layer interface is an important impurity that may contribute to degradation of the mobility. Substitution of TESb for TMSb did not result in any improvement in the purity of the InSb.


1996 ◽  
Vol 421 ◽  
Author(s):  
J. T. Zhu ◽  
A. R. Clawson ◽  
P. K. L. Yu

AbstractWe report the results of the growth of InAsyP1−y /InP and In0.86Ga0.14AS0.51P0.49/ In0.86Ga0.14As0.33P0.67 compressive strained multiple quantum wells (CSMQW) structures grown by low pressure metalorganic chemical vapor deposition (LP-MOCVD). Our studies showed high quality 1.06 μm InAs0.21P0.79/InP CSMQW structure with 6 periods can be obtained when the growth temperature is around 650°C and the pressure in the reactor is about 20 Torr. When the well thickness and composition are tuned for wavelength around 1.30 μm, the quality of this structure degrades. By employing 1.1 μm wavelength, lattice-matched InGaAsP as the barrier layers and setting the growth temperature at 600 °C, high quality 1.30 μm wavelength In0.86Ga0.14AS0.51P0.49/ In0.86Ga0.14As0.33P0.67 CSMQW materials with 10 periods can also be obtained. The materials were characterized with high resolution x-ray rocking curves, room and low temperature photoluminescence (PL). The 15K full-width-at-half-maximums (FWHM) of the PL peaks for 1.06 μm InAs0.21P0.79/InP and 1.30 μm In0.86Ga0.14AS0.51P0.49/ In0.86Ga0.14As0.33P0.67 CSMQW structures are 5.6 meV and 4.97 meV, respectively, which are among the smallest FWHMs reported up to date for these kinds of MOCVD growth materials. Buried heterostructure lasers at 1.3 μm wavelength have been obtained with the CSMQWs as the active layer.


Vacuum ◽  
1990 ◽  
Vol 41 (1-3) ◽  
pp. 715-717 ◽  
Author(s):  
M Nishio ◽  
H Ogawa ◽  
A Yoshida

2006 ◽  
Vol 55 (6) ◽  
pp. 2982
Author(s):  
Zhao Qian ◽  
Pan Jiao-Qing ◽  
Zhang Jing ◽  
Zhou Fan ◽  
Wang Bao-Jun ◽  
...  

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