“…This growth sector appears a little darker within the doped stripes, which is attributed to a higher incorporation of nitrogen on the C-polar facet than elsewhere. 19,20 In this section, three different polytype inclusions were seen. Their starting points, indicated by the red circles, are all located in the (000-1) growth sector.…”
Section: Observation Of Foreign Polytype Formation Andmentioning
confidence: 81%
“…The other two (circles 2 and 3 in Figure 2a) are thin 15R−SiC lamellae, i.e., they do not expand axially in the [000-1] direction. Once formed on the facet, inclusions expand laterally following the step propagation toward the [11][12][13][14][15][16][17][18][19][20] direction and spread all along the crystal diameter. A higher magnification picture of inclusions 1−3 is shown in Figures 2b−d.…”
Section: Observation Of Foreign Polytype Formation Andmentioning
confidence: 99%
“…The consequence is the occurrence of two (000-1) facets at both sides of the section. On the right-hand side facet, three 6H−SiC thin lamellae nucleate, indicated by circles 1−3 (Figure 3a), and expand toward the [11][12][13][14][15][16][17][18][19][20] direction. On the left-hand side facet, a thick 15R−SiC inclusion nucleates (left side of Figure 3).…”
Section: Observation Of Foreign Polytype Formation Andmentioning
confidence: 99%
“…To resolve the geometrical evolution of the crystal, we quantified both normal (along the [000-1] direction) and lateral (along the [11][12][13][14][15][16][17][18][19][20] direction) growth rates. Also, the lateral propagation of the polytype inclusions (A1−A3 and B1− B3 for inclusions 1−3 of crystals A and B, respectively) was systematically evaluated.…”
Section: Observation Of Foreign Polytype Formation Andmentioning
The
nucleation and propagation of foreign polytypes during seeded
sublimation growth of silicon carbide is addressed on a macroscopic
footing, using a coupled experimental and numerical simulation approach.
Experiments are conducted in a contactless growth geometry for different
seed substrates with varying polarity, miscut angle, polytype, and
crystal shape (concave and convex). The interface shape evolution
is tracked by periodic nitrogen marking, which also allows the measurement
of lateral and normal growth rates at any time during growth. Classical
2D nucleation theory is included in modeling the full process, and
this is compared to experiments. We demonstrate that the occurrence
of a foreign polytype is linked to the combined effects of (i) the
presence of the natural {0001} facets and (ii) the minimization of
2D nucleation energy. Areas with a high probability of foreign polytype
nucleation can thus be predicted. Once formed, the progress or disappearance
of foreign inclusions is directly related to their interaction with
the macroscopic growth interface of the crystal.
“…This growth sector appears a little darker within the doped stripes, which is attributed to a higher incorporation of nitrogen on the C-polar facet than elsewhere. 19,20 In this section, three different polytype inclusions were seen. Their starting points, indicated by the red circles, are all located in the (000-1) growth sector.…”
Section: Observation Of Foreign Polytype Formation Andmentioning
confidence: 81%
“…The other two (circles 2 and 3 in Figure 2a) are thin 15R−SiC lamellae, i.e., they do not expand axially in the [000-1] direction. Once formed on the facet, inclusions expand laterally following the step propagation toward the [11][12][13][14][15][16][17][18][19][20] direction and spread all along the crystal diameter. A higher magnification picture of inclusions 1−3 is shown in Figures 2b−d.…”
Section: Observation Of Foreign Polytype Formation Andmentioning
confidence: 99%
“…The consequence is the occurrence of two (000-1) facets at both sides of the section. On the right-hand side facet, three 6H−SiC thin lamellae nucleate, indicated by circles 1−3 (Figure 3a), and expand toward the [11][12][13][14][15][16][17][18][19][20] direction. On the left-hand side facet, a thick 15R−SiC inclusion nucleates (left side of Figure 3).…”
Section: Observation Of Foreign Polytype Formation Andmentioning
confidence: 99%
“…To resolve the geometrical evolution of the crystal, we quantified both normal (along the [000-1] direction) and lateral (along the [11][12][13][14][15][16][17][18][19][20] direction) growth rates. Also, the lateral propagation of the polytype inclusions (A1−A3 and B1− B3 for inclusions 1−3 of crystals A and B, respectively) was systematically evaluated.…”
Section: Observation Of Foreign Polytype Formation Andmentioning
The
nucleation and propagation of foreign polytypes during seeded
sublimation growth of silicon carbide is addressed on a macroscopic
footing, using a coupled experimental and numerical simulation approach.
Experiments are conducted in a contactless growth geometry for different
seed substrates with varying polarity, miscut angle, polytype, and
crystal shape (concave and convex). The interface shape evolution
is tracked by periodic nitrogen marking, which also allows the measurement
of lateral and normal growth rates at any time during growth. Classical
2D nucleation theory is included in modeling the full process, and
this is compared to experiments. We demonstrate that the occurrence
of a foreign polytype is linked to the combined effects of (i) the
presence of the natural {0001} facets and (ii) the minimization of
2D nucleation energy. Areas with a high probability of foreign polytype
nucleation can thus be predicted. Once formed, the progress or disappearance
of foreign inclusions is directly related to their interaction with
the macroscopic growth interface of the crystal.
“…In the literature, O and N impurities originating from contamination are discussed as possible candidates for the creation of donor-like states within the energy gap of lcSiC:H. 2,6,7 From c-SiC it is well known that N is a very good shallow donor impurity, due to its low ionization energy. 28 Unlike the case of unintentionally n-type doped microcrystalline silicon, where the use of gas purifiers during deposition decreased [O] and r d , 29 Finger et al 2 reported that the electrical properties of unintentionally n-type doped lcSiC:H were not affected by gas purifiers. In the present work, although r d covers a very large range-9 orders of magnitude- [O] In the following we discuss two plausible options that might explain the strong increase of r d , which is dominated by an increase of n, without any increase of the donor impurity concentrations.…”
Microcrystalline silicon carbide (lc-SiC:H) deposited by hot wire chemical vapor deposition (HWCVD) and plasma-enhanced chemical vapor deposition (PECVD) provide advantageous optoelectronic properties, making it attractive as a window layer material in silicon thin-film and silicon heterojunction solar cells. However, it is still not clear which electrical transport mechanisms yield dark conductivities up to 10 À3 S/cm without the active use of any doping gas and how the transport mechanisms are related to the morphology of lc-SiC:H. To investigate these open questions systematically, we investigated HWCVD and PECVD grown layers that provide a very extensive range of dark conductivity values from 10 À12 S/cm to 10 À3 S/cm. We found out by secondary ion mass spectrometry measurements that no direct correlation exists between oxygen or nitrogen concentrations and high dark conductivity r d , high charge carrier density n, and low activation energy Ea. Higher r d seems to rise from lower hydrogen concentrations or/and larger coherent domain sizes L SiC . On the one hand, the decrease of r d with increasing hydrogen concentration might be due to the inactivation of donors by hydrogen passivation that gives rise to decreased n. On the other hand, qualitatively consistent with the Seto model, the lower r d and lower n might be caused by smaller L SiC , since the fraction of depleted grain boundaries with higher Ea increases accordingly. Published by AIP Publishing. [http://dx
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