2006
DOI: 10.1016/j.jcrysgro.2005.12.083
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Reflection high-energy electron diffraction study of molecular beam epitaxy growth of Pr2O3 on Si(0 0 1)

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Cited by 11 publications
(11 citation statements)
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“…In this case, the Si atoms reach to the surface. When P O 2 is around 5-6 Â 10 À8 mbar, diffraction patterns due to the two orthogonal cubic domains of Gd 2 O 3 , just as for epitaxial cubic Pr 2 O 3 on Si(0 0 1) [8], are clearly observed. In this system, both cubic domains are [1 0 1] oriented, but the [1 0 1 ] axis of one domain is parallel to Si [11 0] in-plane while the [0 1 0] axis of the other domain is parallel to Si[11 0].…”
Section: Methodsmentioning
confidence: 91%
“…In this case, the Si atoms reach to the surface. When P O 2 is around 5-6 Â 10 À8 mbar, diffraction patterns due to the two orthogonal cubic domains of Gd 2 O 3 , just as for epitaxial cubic Pr 2 O 3 on Si(0 0 1) [8], are clearly observed. In this system, both cubic domains are [1 0 1] oriented, but the [1 0 1 ] axis of one domain is parallel to Si [11 0] in-plane while the [0 1 0] axis of the other domain is parallel to Si[11 0].…”
Section: Methodsmentioning
confidence: 91%
“…NiSi electrodes are fabricated for measuring the electrical properties by using a combination of photolithography and silicidation processes for the top polycrystalline Si layer. [4]. Additional peaks at H ¼ K ¼ 0.90 and 1.83 are clearly observed for samples (a) and (b).…”
Section: Methodsmentioning
confidence: 89%
“…This result indicates that an interdiffusion of atoms occurs during the nucleation and an initial interfacial layer is formed before the formation of the crystalline Pr 2 O 3 phase. The clear pattern of cubic Pr 2 O 3 due to the two orthogonal cubic domains [4], appears only after the thickness reaches more than 2-3 nm, indicating that the interfacial layer is approximately 2 nm thick at this point. The typical interfacial layer thickness, grown under similar conditions, is reported as 1-2 nm in other works [2,4,11].…”
Section: Methodsmentioning
confidence: 95%
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