2018
DOI: 10.1149/2.0031808jss
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Passivation of Surface Recombination at the Si-Face of 4H-SiC by Acidic Solutions

Abstract: We carried out carrier lifetime measurements for 4H-SiC single crystals in aqueous solutions with various pH by the microwave photoconductivity decay method. For both n-and p-type 4H-SiC, carrier lifetimes measured by Si-face excitation were longer in acidic aqueous solutions compared with carrier lifetimes measured in other solutions. On the other hand, for C-face excitation, carrier lifetimes did not depend on immersion solutions. These results indicate that carrier recombination centers at the surface of th… Show more

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Cited by 17 publications
(13 citation statements)
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“…As has been mentioned earlier, the current flow in the I-V measurements is mostly in the low barrier height regions and hence the barrier height reflects those regions only, whereas the C-V measurements gives the average value of the barrier height for the entire surface area of the Schottky contact. More work is needed to further understand the defects in the material and devise preparation approaches such as surface passivation and edge termination for mitigating these effects [21,22]. The effect can be more pronounced in Schottky contacts with large spatial variation of barrier heights.…”
Section: Electrical Measurements On Si and N-type Epitaxial Layersmentioning
confidence: 99%
“…As has been mentioned earlier, the current flow in the I-V measurements is mostly in the low barrier height regions and hence the barrier height reflects those regions only, whereas the C-V measurements gives the average value of the barrier height for the entire surface area of the Schottky contact. More work is needed to further understand the defects in the material and devise preparation approaches such as surface passivation and edge termination for mitigating these effects [21,22]. The effect can be more pronounced in Schottky contacts with large spatial variation of barrier heights.…”
Section: Electrical Measurements On Si and N-type Epitaxial Layersmentioning
confidence: 99%
“…Thus, at the semiconductor–solution interface with no surface states (i.e., there are no states for electrons or holes at the semiconductor surface), the excess charges are spread out inside the semiconductor because the interfacial activity could significantly use up or add to the sparsely available electrons in the semiconductor. Most semiconductors, including N-doped 4H-SiC, have surface states with adsorbed layers, particularly those with adsorbed H and O. , As a result, the potential–distance relationship inside the N-doped 4H-SiC bulk remains flat, and this behavior is more like a metal. As shown in Figure S3, there should be a substantial potential difference in the Helmholtz layer in the solution, and the potential difference inside the 4H-SiC semiconductor is reduced to a small value.…”
Section: Resultsmentioning
confidence: 99%
“…4H-SiC samples of 35, 65 and 120 μm thickness were produced [15] from a commercial 150 μm thick n-type wafer (n 0 = (10±2) × 10 14 cm -3 due to nitrogen doping) grown on a heavily-doped 4H-SiC (0001) substrate at carbon rich conditions (C/ Si ≈ 1.2). The latter feature led to a low Z 1/2 density (<5 × 10 12 cm -3 [16]) in the layers.…”
Section: Samples and Techniquesmentioning
confidence: 99%