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E. Uccelli, M. Bichler, S. Nürnberger, G. Abstreiter, A

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Presentation on theme: "E. Uccelli, M. Bichler, S. Nürnberger, G. Abstreiter, A"— Presentation transcript:

1 Controlled Synthesis of InAs Wires, Dot and Twin-Dot Array configurations by Cleaved Edge Overgrowth
E. Uccelli, M. Bichler, S. Nürnberger, G. Abstreiter, A. Fontcuberta i Morral Nanotechnology 19, 2008

2 What is it all about? Control of size and thereby emission properties of QDs is possible but control of position is more challenging In situ cleaved edge overgrowth to control the nucleation of InAs QDs Uccelli, Bichler, Nürnberger, Abstreiter and Fontcuberta i Morral

3 Cleaved Edge Overgrowth - Fabrication I
Quantum well structures in (001) direction – turn into stripes on a (110) facet which is natural cleavage plane Quantum structures originate at intersection of two or three quantum wells which can be defined with atomic precision – thus this precision is transferred to the lower dimensional structures. Left: L. Pfeiffer et al., Appl. Phys. Lett. 56, 1697 (1990) Right: G. Schedelbeck et al., Science 278, 1792 (1997)

4 Growth of InAs Structures on Cleaved GaAs/AlAs - Fabrication II
AlAs stripes of thicknesses ranging from 3-42 nm with 90 nm GaAs in between Different structures achieved – nanowires, QD chains Stranski-Krastanov growth mode

5 Phenomenological Growth Models
γs = γsf + γf cosφ Layer-by-layer Frank-van der Merve Layer-plus-island Stranski-Krastanov Island Vollmer-Weber γs ≥ γsf + γf + CkBT ln(p0/p) γs < γsf + γf + CkBT ln(p0/p)

6 Mechanism for Growth 1 ML = 2.83 Å
Selective mass redistribution of InAs towards AlAs stripes – consequence of reduced mobility of and lifetime of adatoms on AlAs (110) surface compared to the GaAs (100) surface (around 1 micrometer) In/As adatoms slow down over AlAs regions which increases probability of precipitation and covalent binding on the surface Thickness of InAs material deposited on AlAs region is larger than nominal thickness and will depend on the stripe width (so will onset of formation of InAs QDs) – onset of QD formation occurs at lower thickness than planar case (for Stranski-Krastanov growth model) Slope changes right when QD formation occurs – heigth of QDs is higher than nominal thickness indicating strong migration of InAs from the neighbouring areas The value of the slope is a convolution of the diffusion length on (110) oriented AlAs stripes and on the growing InAs layers Difference in slopes before and after QD formation is geometrical effect due to rearrangement from wires to dots 1 ML = 2.83 Å

7 Twin-Dot Arrays

8 BUT! Also growth on GaAs regions

9 Conclusion Atomic precison of MBE used for positioning of QDs and other structures Technique seems limited to simple geometries because of the use of cleavage planes Small window for preferential growth on AlAs but it is there! Questions?


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