Interface structure and growth mode of quantum wire and quantum dot GaAs-AlAs structures on corrugated (311)A surfaces

被引:30
作者
Ledentsov, NN
Litvinov, D
Rosenauer, A
Gerthsen, D
Soshnikov, IP
Shchukin, VA
Ustinov, VM
Egorov, AY
Zukov, AE
Volodin, VA
Efremov, MD
Preobrazhenskii, VV
Semyagin, BP
Bimberg, D
Alferov, ZI
机构
[1] Tech Univ Berlin, Inst Festkorperphys, D-10623 Berlin, Germany
[2] Univ Karlsruhe, Lab Elektronenmikroskopie, D-76128 Karlsruhe, Germany
[3] Russian Acad Sci, Abraham Ioffe Phys Tech Inst, St Petersburg 194021, Russia
[4] Russian Acad Sci, Inst Semicond Phys, Siberian Div, Novosibirsk 630090, Russia
关键词
quantum dots; corrugated superlattices; (311)A GaAs surface;
D O I
10.1007/s11664-001-0084-1
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
GaAs-AlAs corrugated superlattices (CSL) are formed on spontaneously nanofaceted (311)A surfaces. Using high-resolution transmission electron microscopy (HRTEM) along the [(2) over bar 33] zone axis with an appropriate image evaluation technique to enhance the contrast between GaAs and AlAs we found two distinct lateral periodicities along the [0(1) over bar1] directions for two different CSL layer thickness regimes. For multilayer deposition with GaAs layer thickness exceeding 1 nm the lateral periodicity of 3.2 nm is clearly revealed. The contrast originates from the thickness modulation of both AlAs and GaAs layers with a period of 3.2 nM in the [0(1) over bar1] direction. The corrugation height is about 1 nm and it is symmetric for both upper and lower GaAs-AlAs interfaces. Thicker sections of the thickness-modulated AlAs and GaAs layers of the CSL are shifted by a half period with respect to each other. In the regime when the GaAs deposited average thickness is below 1 nm, which is necessary for complete coverage of the AlAs surface, a lateral periodicity of similar to1.5-2 nm is additionally revealed. We attribute this effect to the formation of local GaAs clusters dispersed on a corrugated (311)A AlAs surface resulting in a local phase reversal of the AlAs surface in their vicinity upon subsequent overgrowth. This reversal can be explained by the same effect as the phase shift, of the surface corrugation upon heteroepitaxy on (311)A. In our model AlAs does not wet the GaAs cluster surface, unless different more energetically favorable scenario is possible. This causes accumulation of AlAs in the vicinity of the GaAs cluster and, as a result, the local phase reversal of the AlAs surface. The AlAs corrugated surface domains with different phases coexist on the surface resulting in an additional periodicity revealed in the HREM contrast modulation. Additionally HRTEM studies indicate that the AlAs-GaAs interface inclination angles in both regimes are 40 degrees and 140 degrees with respect to the flat(311) surface in an agreement with the {331} facet geometry model proposed by R. Notzel, N.N. Ledentsov, L. Daweritz, M. Hohenstein, and K. Ploog [Phys. Rev. Lett. 67, 1812 (1991)].
引用
收藏
页码:463 / 470
页数:8
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