2015
DOI: 10.1016/j.actamat.2015.07.062
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Direct observation of NiSi lateral growth at the epitaxial θ-Ni2Si/Si(1 0 0) interface

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Cited by 14 publications
(39 citation statements)
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References 23 publications
(58 reference statements)
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“…Discussions based on interface energy are not straightforward, due to a lack on experimental data on the interface energy. More recently, Kousseifi et al[35] could quantitatively determine the interface energy for Pt-alloyed NiSi and θ-Ni 2 Si. However, different alloys, or different alloying concentration, can alter the preferential orientation of silicides or change the interface energy through accumulation at the grain-boundaries.…”
mentioning
confidence: 99%
“…Discussions based on interface energy are not straightforward, due to a lack on experimental data on the interface energy. More recently, Kousseifi et al[35] could quantitatively determine the interface energy for Pt-alloyed NiSi and θ-Ni 2 Si. However, different alloys, or different alloying concentration, can alter the preferential orientation of silicides or change the interface energy through accumulation at the grain-boundaries.…”
mentioning
confidence: 99%
“…However, nucleation at the interface and/or at the triple junction, as well as the lateral growth along interface play an important role in the formation of silicide. This is particularly true for very thin films [47] and may lead to much more complex microstructures. Anyway, for thickness larger than about 10 nm, the nucleation and lateral growth end to a continuous layer which grows then essentially in a one-dimensional manner.…”
Section: Discussionmentioning
confidence: 99%
“…The TEM images (Fig. 7) allow a direct comparison with these models and the analytical solutions [61,63,67,68] have been used to fit the TEM images instead of the numerical simulation developed by Lucenko et al [11] and Vovk et al [9]. Moreover Fig.…”
Section: Lateral Growth: Comparison Between Models and Morphologies Dmentioning
confidence: 99%
“…The main assumptions of these models are: (1) the asymmetrical position of the NiSi particle with respect to the θ-Ni2Si /Si interface is due to the matter conservation and to the volume change during the reaction between θ-Ni2Si and Si, (2) the mechanical equilibrium of the interfacial energies is responsible for the particle shape (3) the Ni and Si interdiffusion along interfaces is assumed to drive the kinetics of the fast lateral growth; the elements Ni and Si are thus considered to diffuse in opposite directions along the Si/NiSi and θ-Ni2Si/NiSi interfaces, and (4) the driving force for the flux of the diffusing element along the interface is the gradient of the chemical potential difference due to the gradient of curvature. In these models [61,63,67,68], the steady state shape of the moving interface and its velocity are calculated from the flux and the mass conservation condition across the moving interface and the boundaries. In addition to reproduce the global shape of the precipitaes, the model developed by Pasichnyy and Gusak [63] allows the initial interface (θ-Ni2Si/Si) to be deformed and to become curved.…”
Section: Lateral Growth: Comparison Between Models and Morphologies Dmentioning
confidence: 99%
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