2019
DOI: 10.1016/j.jcrysgro.2019.03.027
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Formation and multiplication of basal plane dislocations during physical vapor transport growth of 4H-SiC crystals

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Cited by 16 publications
(9 citation statements)
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“…It is reported that during the PVT growth of 4H-SiC single crystals, a large amount of thermoelastic shear stress caused by a temperature gradient in the crystal is introduced in the nonfacet region, while the facet region is almost none, which may forbid the expansion of SFs (3,3) generated in the nonfacet region. In order to verify the stress distribution across the facet and nonfacet regions, we plot the FTO-peak mapping of the region in Figure (b).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…It is reported that during the PVT growth of 4H-SiC single crystals, a large amount of thermoelastic shear stress caused by a temperature gradient in the crystal is introduced in the nonfacet region, while the facet region is almost none, which may forbid the expansion of SFs (3,3) generated in the nonfacet region. In order to verify the stress distribution across the facet and nonfacet regions, we plot the FTO-peak mapping of the region in Figure (b).…”
Section: Resultsmentioning
confidence: 99%
“…35 In addition, the FTO-peak positions of SFs (3,3) tending to abruptly shift toward higher wavenumbers always occurs, implying that the compressive strain exists in SFs (3,3). 38,40 This indicates that the shear stress exerted in the nonfacet region is released by the formation and expansion of SFs (3,3), due to the low formation energies of SFs in n-type 4H-SiC. Once the expansion of SFs (3,3) reaches the interface of the facet and nonfacet regions, the compressive stress impedes the expansion of SFs (3,3).…”
Section: Resultsmentioning
confidence: 99%
“…This is also true for the radial temperature gradient. It was demonstrated numerically and experimentally that, from the shoulder region of a crystal, BPD arrays form and propagate into the crystal [ 177 , 178 ]. Therefore, low radial and axial gradients are preferred, without either inducing a concave growth interface or reducing the mass transport between source and seed too much.…”
Section: Silicon Carbide Materialsmentioning
confidence: 99%
“…The physical model is also supported by Raman measurements, as shown in figure 4(c). Raman spectra along the growth direction indicate that the peak position of the E 2 mode shifts abruptly where bunched BPDs existed, indicating that the bunched BPDs are introduced at the domed surface and are hardly introduced from the side surfaces of the grown crystals [49]. The most plausible location where BPDs are introduced would be the shoulder regions of growth crystals.…”
Section: Generation Of Dislocationsmentioning
confidence: 99%