共查询到18条相似文献,搜索用时 55 毫秒
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利用低能电子衍射(LEED)、X射线光电子能谱(XPS)、电子能量损失谱(EELS)、紫外光电子能谱(UPS),对室温下Mn在GaAs(100)4×1表面的淀积过程进行了研究。研究结果表明,当锰的覆盖度θ≥0.25nm时,LEED图案完全消失,表明Mn没有生长成单晶。LEED,EELS的结果都表明淀积初期是层状生长的。对XPS的Ga2p3/2,As2p3/2的峰形、强度进行分析,可以知道在很小的覆盖度下,Mn就与衬底反应。置换出的Ga被局限在离原来的界面约3nm
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采用同步辐射光电子能谱(SRPES)结合扫描电子显微镜(SEM)和称量法,研究了中性(NH4)2S溶液钝化GaAs(100)表面,并与常规(NH4)2S碱性溶液钝化方法进行了比较- SRPES结果表明该处理方法可以产生较厚的Ga硫化物层和较强的Ga—S键,Ga的硫化物有好的稳定性-称量法表明该方法有更低的腐蚀速率-SEM结果表明该方法钝化处理的GaAs表面所产生的腐蚀坑数目少,直径小-
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利用同步辐射光电发射和铁磁共振(FMR)研究了Co/GaAs(100)界面形成以及Co超薄膜的磁性质.结果表明,在低覆盖度(约为0.2nm)下,Co吸附原子与衬底发生强烈的界面反应,在覆盖度为0.9nm时,形成稳定的界面.从衬底扩散出的Ga原子与Co覆盖层合金化,而部分As原子与Co原子发生反应,形成稳定的键合,这些反应产物都停留在界面处很窄的区域(0.3—0.4nm)内.另一部分As原子偏析在Co覆盖层表面.结合理论模型,详细地讨论了界面结构及Ga,As原子的深度分布.FMR结果表明,生长的Co超薄膜具
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为了有效降低GaAs半导体表面态密度,提出了采用正十八硫醇(ODT,CH3[CH2]17SH)进行GaAs表面钝化的方案。首先,分别对GaAs(100)晶片进行了常规硫代乙酰胺(TAM,CH3CSNH2)钝化和正十八硫醇钝化,通过X射线光电子能谱(XPS)对比分析了钝化前后晶片表面的化学成分,然后利用光致发光光谱(PL)对正十八硫醇处理的GaAs(100)晶片进行了钝化时间的优化,最后通过扫描电子显微镜(SEM)测试了钝化前后的晶片表面形貌。实验结果表明:采用正十八硫醇钝化的GaAs(100)表面,相比常规硫代乙酰胺钝化方案,具有更低的氧化物含量和更厚的硫化层厚度;室温钝化条件下,钝化时间越长,正十八硫醇的钝化效果越好,但PL强度在钝化超过24 h后基本达到稳定,最高PL强度提高了116%;正十八硫醇钝化的GaAs(100)晶片具有良好的表面形貌,表面形成了均匀、平整的硫化物钝化层。数据表明正十八硫醇是钝化GaAs(100)表面一种非常有效的技术手段。 相似文献
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为实现GaAs表面的钝化,以Na2S、(NH4)2S、CH3CSNH2为主要研究对象,通过对比实验研究得出较为理想的湿法钝化液。通过光致发光(PL)谱研究了(NH4)2S 叔丁醇、CH3CSNH2 NH4OH、CH3CSNH2 叔丁醇三种不同含硫溶液钝化(100)GaAs表面后的发光特性。PL谱测试发现,(NH4)2S 叔丁醇饱和溶液处理过的(100)GaAs表面光致发光强度最强,PL谱的相对发光强度是未做钝化处理的10倍左右。因此得出(NH4)2S 叔丁醇饱和溶液是较为理想的(100)GaAs表面钝化液。 相似文献
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建立了一种硫钝化GaAs(100)表面的新方法,即CH3CSNH2/NH4OH溶液处理,应用同步辐射光电子能谱(SRPES)和X射线光电子能谱(XPS)表征了该钝化液处理的n-GaAs(100)表面的成键,特性和电子态.结果表明,经过处理的n-GaAs(100)表面,S既与As成键也与Ga成键,形成S与GaAs的新界面,并且Ga和As的氧化物被移走,这标志着CH3CSNH2/NH4关键词: 相似文献
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A. Sharma S. Tripathi N. Lakshmi P. Sachdev T. Shripathi 《Solid State Communications》2009,149(25-26):1033-1038
The structural, magnetic and transport properties measurements carried out on Co thin films deposited by electron beam evaporation on GaAs substrate as a function of layer thickness ranging from 50 Å to 1000 Å are presented here. Structural measurements show the film to be amorphous in nature at lower thickness which becomes crystalline at higher thickness. Magnetic measurements show an increase in saturation magnetization (MS) with film thickness. MS values are found to vary from 521 emu/cm3 to 1180 emu/cm3 for thicknesses ranging from 50 Å to 1000 Å. The coercivity and saturation field value shows a systematic decrease up to 600 Å thickness and increase thereafter. Various microstructural parameters were also calculated using GIXRR technique. A clear grain growth is observed in AFM technique with film thickness and its influence on transport properties was also seen. Different surface morphology and magnetic domain structures were obtained on different thin film samples by AFM and MFM techniques, respectively. XPS measurements reveal formation of CoAs phase at the interface between Co and GaAs. All these results are discussed and interpreted in detail in this communication. 相似文献
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INTERFACE FORMATION OF Ge/ZnSe(100) AND Ge/ZnS(111) HETEROJUNCTIONS STUDIED BY SYNCHROTRON RADIATION PHOTOEMISSION 下载免费PDF全文
The microscopic evolution of interface formation between Ge and Ⅱ-Ⅵ compounds such as ZnSe and ZnS single crystals has been studied by synchrotron radiation photoemission spectroscopy and low energy electron diffraction. Core level intensity measurements from the substrate as well as from the overlayer show a nearly ideal two-dimensional growth mode for the deposition of Ge on ZnSe(100) surface. How-ever, there is a certain deviation from the ideal two-dimensional mode in the case of Ge/ZnS(111) due to the diffusion of substrate atoms into Ge overlayer. Surface semi-tire core level spectra indicate that the reaction of Ge with S atoms at Ge/ZnS(111) interfaces is much stronger than that of Ge with Se atoms at Ge/ZnSe(100) interfaces. 相似文献
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The interface formation and electronic structures of the Mn/GaP(100) interface are studied with synchrotron radiation photoemission, At the early stage of Mn deposition, Mn covers the whole GAP(100) surface. With the increase of coverage, Ga atoms can be exchanged by Mn atoms and diffuse into the Mn overLaycr. However, P atoms remain always near the interracial region. A sigaificant difference of the electronic structures is observed between the ultra-thin and the thick Mn films. The explanations for this are given in the text. 相似文献
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