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首页> 外文期刊>Physical Review, B. Condensed Matter >Electronic structure of the N donor center in 4H-SiC and 6H-SiC - art. no. 085206
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Electronic structure of the N donor center in 4H-SiC and 6H-SiC - art. no. 085206

机译:4H-SiC和6H-SiC中N供体中心的电子结构-艺术。没有。 085206

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摘要

In this paper, we present high-frequency (95 GHz) pulsed electron paramagnetic resonance (EPR) and electron nuclear double resonance (ENDOR) measurements on the nitrogen (N) donor in 4H-SiC (k site) and 6H-SiC (h, k(1), and k(2) sites according to the accepted classification). From the isotropic (a) and anisotropic (b) hyperfine interaction of the unpaired electron spin of the donor with the C-13 (35% C-13-enriched samples were used) and Si-29 nuclei, the distribution of the electronic wave function of the N donor is determined. It is found that this wave function is quite different in the two polytypes because the spin-density distribution over the C-13 and Si-29 nuclei differs between the 4H and 6H polytypes. A similar conclusion was derived from the EPR line broadening of the N donor in C-13-enriched 4H- and 6H-SiC compared with nonenriched crystals. The main part of the spin density in 4H-SiC is located on the Si sublattice and the wave function contains a relatively large portion of Si p character. A tentative assignment is proposed for five ENDOR lines. For the three sites in 6H-SiC, the main part of the spin density is located on the C sublattice and the wave function is built Mostly of s-like C atomic orbitals. Comparing the three sites in 6H-SiC, the It site wave function has the largest delocalization and is most isotropic. The k(2) Site wave function is most localized and less isotropic. The largest part of the spin density is located far into the crystal. The difference in behavior of the wave function in 4H and 6H polytypes seems to find its origin in the difference in their conduction-band structure. Our results indicate that the conduction-band minima in 4H-SiC (bottom of the conduction bands) are mainly Si-like, whereas in 6H-SiC the conduction-band minima are mostly C-like. [References: 37]
机译:在本文中,我们对4H-SiC(k位置)和6H-SiC(h)中的氮(N)供体进行了高频(95 GHz)脉冲电子顺磁共振(EPR)和电子核双共振(ENDOR)测量。 ,k(1)和k(2)网站)。从供体的未配对电子自旋与C-13(使用了35%的C-13富集样品)和Si-29原子核的各向同性(a)和各向异性(b)的超精细相互作用中,电子波的分布确定N供体的功能。发现在两个多型体中,这种波函数是完全不同的,因为在4H和6H多型体中,C-13和Si-29核上的自旋密度分布不​​同。与未富集晶​​体相比,富C-13的4H-和6H-SiC中N供体的EPR谱线拓宽也得出了类似的结论。 4H-SiC中自旋密度的主要部分位于Si子晶格上,并且波函数包含相对较大的Si p特性部分。建议为5条ENDOR线分配一个临时作业。对于6H-SiC中的三个位点,自旋密度的主要部分位于C子晶格上,并且波函数主要由s形C原子轨道构成。比较6H-SiC中的三个位点,It位点波函数具有最大的离域和各向同性。 k(2)站点波函数最局限,各向同性较小。自旋密度的最大部分位于晶体的远处。在4H和6H多型中,波函数的行为差异似乎是由其导带结构的差异引起的。我们的结果表明,在4H-SiC(导带的底部)中的导带最小值主要为Si形,而在6H-SiC中,导带最小值为大多数C型。 [参考:37]

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