Suppression of large island formation in InAs/InGaAs dot-in-a-well structures with periodic AsH3 interruption
Kim, Jungsub; Yang, Changjae; Ahn, Eungjin; Yoon, Euijoon; Lee, Yongsoo; Cheong, Hyeonsik; Choi, Wonjoon
Republic of Korea

Self-assembled InAs/GaAs quantum dots (QDs) have been widely investigated due to their promising applications such as laser diodes for optical fiber communication, etc. However, the 1.3 μm QD laser grown by metal organic chemical vapor deposition (MOCVD) has not been demonstrated yet, because emission wavelength to 1.3 μm is difficult to obtain due to the formation of dislocations across the interface or due to the relaxed large islands that degrade optical properties.
In present work, we grew InAs QDs by MOCVD with a new growth technique, namely periodic AsH3 interruption (PAI) method, in order to suppress the formation of relaxed large islands. In contrast to the conventional method of QD growth, the supply of AsH3 was periodically interrupted while trimethylindium was introduced into the reactor continuously. By using this method, the growth surface could be modulated from As-stabilized surface to In-stabilized one, resulting in the uniform strain distribution and the increase in In adatom migration length. Therefore, the homogeneous nucleation and uniform QD growth could be promoted in addition to reducing the amount of excess As known to cause dot coalescence. In order to demonstrate these effects, we varied the AsH3 interruption time at fixed total amount of source supply. With long interruption times, large islands were formed. This phenomenon was also occurred with short interruption times, because sufficient times were not provided to modulate the surface condition. On the other hand, the formation of large islands was suppressed completely with the intermediate interruption time (~4 s). As a result, the PL peak intensity was significantly enhanced in comparison to the conventional QD growth method. . In addition, we controlled the composition and thickness of InGaAs well layers in order to tune the emission wavelength. The redshift of the emission wavelength above 1.38 μm was successfully achieved without broadening in linewidth.
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