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Photo EPR Study of Trapping and Recombination Processes in Semi-Insulating 4H-SiC Crystals as Function of Temperature

机译:作为温度函数的半绝缘4H-SIC晶体中捕获和重组过程的照片EPR研究

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Photo-Electron Paramagnetic Resonance (photo-EPR) measurements of semi-insulating (s.-i.) 4H SiC have been made at 37 GHz including photo excitation and photo quenching techniques in the temperature interval from 77 K to 50 K. At T=77 K in the dark the EPR spectrum consists of a low intensity line due to boron on the cubic lattice site and a single line with isotropic g{sub}(||)=g{sub}⊥=2.0025 due to a carbon-related surface defect. During illumination with ultraviolet light the EPR lines of hexagonal boron and cubic nitrogen appear in the EPR spectrum and persist after the illumination is removed. Subsequent illumination of the sample with sub-band gap, visible, light resulted in the quenching of the EPR lines from nitrogen and appearance of the I{sub}(P1) EPR line with g{sub}(||)=2.0048, g{sub}⊥=2.0030 caused by direct transfer of electrons from nitrogen donor to the P1 center. The lifetime of the photo-generated carriers trapped by the P1 centers is found to be more than 15-20 hours after the photo-excitation was turned off. The deep donor P1 local center is suggested to be the as yet unidentified deep level located at E{sub}C-1.1 eV which pins the Fermi level in this sample at this energy in the dark. As the temperature is lowered from 77K and the quasi Fermi level positions reach shallow donor and acceptor states, an additional EPR line, I{sub}D, with g{sub}(||)= 2.0063, g{sub}⊥=2.0006, appears at 50 K in the excitation EPR spectrum and is attributed to the antisite defect (Si{{sub}c}sup)- with an energy level shallower than nitrogen. At the same time the ratio of the photo-excited EPR line intensities responsible for boron on the cubic and hexagonal sites, (I{sub}B){sup}k: (I{sub}B){sup}h, returns to the value observed at 77 K and becomes equal to 0.4 at 50 K, showing that the concentration of boron in the hexagonal site is higher than on the cubic site.
机译:光的电子顺磁共振(光EPR)半绝缘(s.-i.)4H碳化硅的测量已在37 GHz的由包括的照片激发和相片淬火技术在温度间隔从77°K至50 K.在T = 77°K在黑暗中EPR光谱由低强度线的由于硼立方晶格位置上,并且具有各向同性克{子}(||)= G {}子⊥= 2.​​0025单行由于碳有关表面缺陷。在用紫外线照射光六方氮化硼和立方氮的EPR行显示在EPR光谱和所述照明被移除之后仍然存在。与子带隙的样本随后光照,可见光,光导致从I {}子(P1)与EPR {克子}线(||)的氮和外观EPR线的淬火= 2.0048,克{子}⊥= 2.​​0030由从氮供体直接将电子转移到P1中心。由P1中心截留在光生载流子的寿命被发现是超过15-20小时光激发关闭后。深施主P1局部中心被建议为位于E {}子C-1.1eV的其中销在该能量在黑暗中在该样品中的费米能级的身份不明的深能级。随着温度从77K降低,准费米能级的位置达到浅施主和受主态,附加EPR线,I {}亚d,以克{子}(||)= 2.0063,G {}子⊥= 2.​​0006出现在激发EPR谱图50 K和归因于反位缺陷(SI {{子}℃} SUP) - 具有比氮的能级浅。同时负责对立方和六方位点,(I {子} B){SUP} K和硼的光激发EPR线强度的比值:(I {子} B){SUP}小时,返回到的值在77°K和观察变得等于0.4,在50 K,示出了硼的六角形部位中的浓度比在立方站点更高。

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