Author
Listed:
- JIANHUA SHEN
(Surface Physics Laboratory (National Key Laboratory) and Department of Physics, Fudan University, Shanghai 200433, China)
- PING JIANG
(Surface Physics Laboratory (National Key Laboratory) and Department of Physics, Fudan University, Shanghai 200433, China)
- XIDE XIE
(Surface Physics Laboratory (National Key Laboratory) and Department of Physics, Fudan University, Shanghai 200433, China)
Abstract
AlAs(001) is compared with GaAs(001) byab initiopseudopotential total energy calculation. The results show that either similarities or differences in the stability of the surface reconstructions are obvious. On the Al-rich AlAs surface the reconstruction (2×1)/c (2×2) has an obvious energetic advantage. In this reconstruction the topmost Al atoms abnormally locate below the As atomic layer. Besides, on the As-rich GaAs surface a metastable reconstruction phase ofγ(2×4)appears if the surface coverage of As atoms is less than 1, while on the AlAs surface it is fully dimerized (2×1) phase more stable. In addition the thermodynamical analysis also indicates that in the mid-temperature range of MBE growth (e.g. 600°C withAs2pressure of2 × 10-6τ) this (2×1) phase is stable. Further calculations show that 0.2–1 monolayer of Ga atoms deposited on AlAs surface will result inγ(2×4)phase rather than (2×1) phase, while the deposited Ga atoms on the AlAs surface do not go below the topmost As atomic layer. The plausible conclusion is that formation of (2×1) phase on As-rich AlAs surface and the inner location of Al atoms on Al-rich (2×1)/c(2×2) reconstruction surface could be closely related to the obviously different modes of MBE growth on AlAs and GaAs surface, in the mid-temperature range.
Suggested Citation
Jianhua Shen & Ping Jiang & Xide Xie, 1999.
"THE DIFFERENCE BETWEEN THE SURFACE RECONSTRUCTIONS OF AlAs(001) AND GaAs(001),"
Surface Review and Letters (SRL), World Scientific Publishing Co. Pte. Ltd., vol. 6(06), pages 1167-1171.
Handle:
RePEc:wsi:srlxxx:v:06:y:1999:i:06:n:s0218625x99001293
DOI: 10.1142/S0218625X99001293
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