2003
DOI: 10.1063/1.1566455
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Positioning of self-assembled Ge islands on stripe-patterned Si(001) substrates

Abstract: Abstract:Self-assembled Ge islands were grown on stripe-patterned Si (001) substrates by solid source molecular beam epitaxy. The surface morphology obtained by atomic force microscopy (AFM) and cross-sectional transmission electron microscopy images (TEM) shows that the Ge islands are preferentially grown at the sidewalls of pure Si stripes along [-110] direction at 650 o C or along the trenches, whereas most of the Ge islands are formed on the top terrace when the patterned stripes are covered by a straine… Show more

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Cited by 99 publications
(62 citation statements)
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“…Such f111g pyramids are the result of a shape transition from domes, accompanied by a substantial increase of the a=r. Molecular dynamics (MD) simulations and elasticity-theory calculations are used to explain the role played by the substrate pattern in altering the strain distribution and favoring coherence at high a=r.Patterned Si(001) substrates with two-dimensionally (2D) periodic pits along two orthogonal h110i directions were obtained by holographic lithography and reactive ion etching [16,17]. To create a well-defined starting surface, a 130 nm thick Si buffer layer was grown with 0:05 nm=s while ramping the temperature from 450 C to 600 C. On sample A only the Si buffer was deposited, whereas samples B and C received in addition 5 and 7 monolayers (ML) of Ge, respectively, which were deposited at 620 C with 0:005 nm=s and 7 s growth interruption after each ML [16].…”
mentioning
confidence: 99%
“…Such f111g pyramids are the result of a shape transition from domes, accompanied by a substantial increase of the a=r. Molecular dynamics (MD) simulations and elasticity-theory calculations are used to explain the role played by the substrate pattern in altering the strain distribution and favoring coherence at high a=r.Patterned Si(001) substrates with two-dimensionally (2D) periodic pits along two orthogonal h110i directions were obtained by holographic lithography and reactive ion etching [16,17]. To create a well-defined starting surface, a 130 nm thick Si buffer layer was grown with 0:05 nm=s while ramping the temperature from 450 C to 600 C. On sample A only the Si buffer was deposited, whereas samples B and C received in addition 5 and 7 monolayers (ML) of Ge, respectively, which were deposited at 620 C with 0:005 nm=s and 7 s growth interruption after each ML [16].…”
mentioning
confidence: 99%
“…For epitaxial heterostructures, the local surface curvature and the mechanical relaxations strongly influence the Ge QDs shape and position [3]. The chemical potential µ [10] allows estimating the most favourable nucleation sites from the thermodynamic point of view.…”
Section: Modellingmentioning
confidence: 99%
“…Obviously, two values of L agree with the theoretical prediction that the surface diffusion length of Ge increases with the Ge growth rate decreasing. 26 With the growth rate v fixed at 0.05 Å/s, by changing the growth temperature (540 ∼ 620…”
Section: -4mentioning
confidence: 99%