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Characterization of Inhomogeneity in SiO_2 Films on 4H-SiC Epitaxial Substrate by a Combination of Fourier Transform Infrared Spectroscopy and Cathodoluminescence Spectroscopy

机译:傅里叶变换红外光谱和阴极荧光光谱相结合表征4H-SiC外延衬底上SiO_2薄膜的不均匀性

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We measured Fourier transform infrared (FT-IR) and cathodoluminescence (CL) spectra of SiO_2 films with various thicknesses, grown on 4H-SiC substrates. The appearance of broad phonon modes at ~1150-1250 cm~(-1) in p-polarized light and their disappearance in s-polarized light confirmed that the phonon modes at ~1150-1250 cm~(-1) originated from surface polaritons (SPPs). For the thin SiO_2 film (8-nm thick), the peak frequency of the transverse optical (TO) phonon in the SiO_2 film on the 4H-SiC substrate was observed at ~1080 cm~(-1) and was higher than that in SiO_2 films on the Si substrate (1074 cm~(-1)). This suggested that the thin SiO_2 film (8-nm thick) is under compressive stresses at the interface between the SiO_2 film and SiC substrate. On the other hand, for the thick SiO_2 films (85 and 130-nm thick), the TO phonon peak frequency tended to shift toward lower frequencies with increasing oxide layer thickness. The CL measurement indicated that the CL peak intensity at ~640 nm, attributed to non-bridging oxidation hole centers (NBOHCs), became stronger with increasing oxide layer thickness, relative to that of the CL peaks at ~460 and 490 nm due to oxygen vacancy centers (OVCs). By comparing the FT-IR and CL measurements, we concluded that the TO phonon red-shift with increasing oxide layer thickness can mainly be attributed to an increase in inhomogeneity with increasing oxide layer thickness for the thick SiO_2 films.
机译:我们测量了在4H-SiC衬底上生长的各种厚度的SiO_2薄膜的傅里叶变换红外(FT-IR)和阴极发光(CL)光谱。 p偏振光在〜1150-1250 cm〜(-1)处的宽声子模的出现以及s偏振光的消失,证实了〜1150-1250 cm〜(-1)处的声子模来自表面极化子(SPPs)。对于厚度为8nm的SiO_2薄膜,在4H-SiC衬底上SiO_2薄膜中的横向光学(TO)声子的峰值频率在〜1080 cm〜(-1)处观察到,并且高于SiO_2薄膜在Si衬底上(1074 cm〜(-1))。这表明SiO_2薄膜(8纳米厚)在SiO_2薄膜和SiC衬底之间的界面处处于压缩应力下。另一方面,对于厚的SiO_2膜(85和130nm厚),随着氧化物层厚度的增加,TO声子的峰值频率趋于向更低的频率偏移。 CL测量表明,归因于非桥接氧化孔中心(NBOHCs)的〜640 nm处的CL峰强度随着氧化物层厚度的增加而变得更强,相对于〜460和490 nm处的CL峰因氧而增加空缺中心(OVC)。通过比较FT-IR和CL测量,我们得出结论:随着氧化层厚度的增加,TO声子红移​​随氧化层厚度的增加而增加,这主要归因于不均匀性的增加。

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