2014
DOI: 10.1063/1.4892658
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In-situ high resolution transmission electron microscopy observation of silicon nanocrystal nucleation in a SiO2 bilayered matrix

Abstract: Solid-state nucleation of Si nanocrystals in a SiO 2 bilayered matrix was observed at temperatures as low as 450 C. This was achieved by aberration corrected high-resolution transmission electron microscopy (HRTEM) with real-time in-situ heating up to 600 C. This technique is a valuable characterization tool especially with the recent interest in Si nanostructures for light emitting devices, non-volatile memories, and third-generation photovoltaics which all typically require a heating step in their fabricatio… Show more

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Cited by 9 publications
(7 citation statements)
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“…The isoconcentration surfaces were defined with a voxel size of 1 nm and a delocalization value of x = 3 nm, y = 3 nm, z = 3.5 nm. The mass spectra used in the reconstruction are shown in Supporting Information (Figure S1).The reconstructions indicate that the Si NCs were well-separated from each other in 3D, despite the Si-rich oxide film being deposited by cosputtering of Si and SiO 2 targets, which is different from creating a multilayer structure of Si-rich oxide and SiO 2 films that is known to create well-distributed Si NCs. , In the sliced images, the codoped sample has more B and P enrichment at the position where the local Si density is high compared to solely doped samples. This B and P enrichment is more prominent when the annealing temperature is increased from 1050 to 1250 °C (Supporting Information, Figure S2, for 3D reconstructions of codoped Si NCs in BPSG annealed at 1050 and 1250 °C).…”
Section: Resultsmentioning
confidence: 99%
“…The isoconcentration surfaces were defined with a voxel size of 1 nm and a delocalization value of x = 3 nm, y = 3 nm, z = 3.5 nm. The mass spectra used in the reconstruction are shown in Supporting Information (Figure S1).The reconstructions indicate that the Si NCs were well-separated from each other in 3D, despite the Si-rich oxide film being deposited by cosputtering of Si and SiO 2 targets, which is different from creating a multilayer structure of Si-rich oxide and SiO 2 films that is known to create well-distributed Si NCs. , In the sliced images, the codoped sample has more B and P enrichment at the position where the local Si density is high compared to solely doped samples. This B and P enrichment is more prominent when the annealing temperature is increased from 1050 to 1250 °C (Supporting Information, Figure S2, for 3D reconstructions of codoped Si NCs in BPSG annealed at 1050 and 1250 °C).…”
Section: Resultsmentioning
confidence: 99%
“…This could either mean that the Si NCs are penetrating through the adjacent 1.8 nm SiO 2 layers as suggested by Di et al [24] or there could be an extensive nanocrystalline Si network within the SRO layers making the Si NCs non-spherical in shape. Furthermore, if the Si NCs are confined well within the layers, Si quantum well type structures could also be a possibility [25]. In HRTEM it is often difficult to find the true shape of the individual Si NCs, because limited information is provided to the viewer along the third dimension (depth) [25], [26].…”
Section: B High Resolution Transmission Electron Microscopymentioning
confidence: 99%
“…Furthermore, if the Si NCs are confined well within the layers, Si quantum well type structures could also be a possibility [25]. In HRTEM it is often difficult to find the true shape of the individual Si NCs, because limited information is provided to the viewer along the third dimension (depth) [25], [26]. The shape has been suggested to be elliptical or even more eccentric as suggested by a few TEM studies [25]- [28].…”
Section: B High Resolution Transmission Electron Microscopymentioning
confidence: 99%
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“…growth of metal nanocrystals and nanoparticles. 33,34 Recent advances allowing time-resolved investigations of self-assembly processes through atomic resolution and single-atom sensitivity include direct imaging of the dynamics of Si 6 clusters embedded in graphene pores, 35 observation of the trapping of metal atoms in graphene, 36 capture of atomic-level random walks of a defect in graphene, 37 and direct visualisation of small clusters of gold atoms. [38][39][40][41] Nonetheless, imaging the early stage of a nanocrystallisation process in real-time and in real-space is challenging and little is known about growth rates of nuclei, the minuscule clusters made of a few atoms formed in the earliest stage of nanocrystal synthesis.…”
mentioning
confidence: 99%