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book of abstracts - IM2NP

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A B S T R A C T S THURSDAY, JULY 1 N A N O S E A 2 0 1 0<br />

2 – Here we present clear experimental evidence for the formation <strong>of</strong> larger domes prior to smaller pyramids<br />

at growth temperatures (Tg) smaller than 675°C and for an "overcritical" behavior <strong>of</strong> the wetting layer<br />

(WL).These findings allow us to sort out thermodynamic and kinetic paths in the early stages <strong>of</strong> quantum dot<br />

formation. The results are obtained from systematic investigations <strong>of</strong> atomic force microscopy (AFM) and<br />

photoluminescence (PL) on samples grown by molecular beam epitaxy. By implementing a Ge gradient over<br />

4” wafers we achieved an extremely high deposition resolution <strong>of</strong> 0.025 monolayers (ML). At Tg =700°C we<br />

observe dome formation at Θ = 4.2 ML, while pyramids appear later, i.e. at Θ > 4.38 ML. The dome<br />

formation is initiated by a Ge transfer <strong>of</strong> 1 ML from the WL to the islands, as determined from the abrupt<br />

shift <strong>of</strong> the WL PL at the onset <strong>of</strong> the island PL. At Tg = 625°C the common dot formation sequence is<br />

observed. Mounds and small pyramids form already at about 2 ML followed by the nucleation <strong>of</strong> domes at<br />

4.9 ML. In order to understand whether the domes are actually stable prior to pyramids, accurate density<br />

functional theory calculations <strong>of</strong> surface energies and finite element method simulations <strong>of</strong> the elastic<br />

energies were performed, taking particular care in determining the total energy variations in the first few<br />

MLs <strong>of</strong> the WL. By a morphological phase diagram we both confirmed the early stability <strong>of</strong> the Ge-rich<br />

domes and the depletion <strong>of</strong> the WL at their onset, also addressing the appearance first <strong>of</strong> pyramids at 625°C<br />

to be a kinetic effect, leading to metastable islands.<br />

3 – An experimental pro<strong>of</strong> for this prediction is obtained from extensive annealing experiments. After<br />

annealing at 700°C pyramids grown with Θ < 3.2 ML at 625°C form back to a completely flat WL, while for<br />

Θ > 3.2 ML domes are formed. Thus, we conclude that the critical WL thickness (tc) for stable island<br />

nucleation is about 3.2 ML. At the same tc domes are formed if we anneal an overcritical WL grown at<br />

700°C. Finally, we would especially like to highlight the strong similarities between dot formation in SiGe<br />

and III/V systems.<br />

18H10-18H30<br />

Formation and Localization <strong>of</strong> GeSi Quantum Dots on vicinal surfaces: a<br />

Scanning Tunneling Microscopy Characterization.<br />

L. PERSICHETTI, A. SGARLATA, M. FANFONI, A. BALZAROTTI (Department <strong>of</strong><br />

Physics, University <strong>of</strong> Roma “Tor Vergata” - Via della Ricerca Scientifica, 1 Roma, Italy).<br />

persichetti@roma2.infn.it<br />

1 – Introduction<br />

Due to the potential applications in novel nanostructured devices, the Stranski-Krastanov growth <strong>of</strong> ordered<br />

self-assembled islands in strained heteroepitaxial systems is a topic attracting ever-increasing interest.<br />

A natural model system is Ge on vicinal Si(001), which allows us to tune both the energetic and the kinetic<br />

factors governing the growth <strong>of</strong> individual nanostructures by changing the substrate miscut [1].<br />

2 – Abstract<br />

A complete description <strong>of</strong> Ge growth and ordering processes on vicinal Si(001) surfaces in the angular<br />

miscut range 0°-8° is presented. The key role <strong>of</strong> substrate vicinality is clarified from the very early stages <strong>of</strong><br />

Ge deposition up to the nucleation <strong>of</strong> 3D islands [2]. By a systematic scanning tunnelling microscopy<br />

investigation we are able to explain the competition between step-flow growth and 2D nucleation and the<br />

progressive elongation <strong>of</strong> the 3D islands along the miscut direction [110].<br />

102

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