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1.
利用同步辐射光电子能谱(SRPES)和X射线光电子能谱(XPS)技术,系统研究了室温下Fe/ZnO界面形成过程中Fe薄膜与氧结尾的ZnO(000 1 )衬底之间的相互作用,结果显示初始沉积的Fe明显被表面氧氧化为Fe2+离子,在Fe覆盖度为0—3 nm的范围内,分别观察到与界面电荷传输、化学反应以及薄膜磁性相关的三个有意义的临界厚度,这一结果将有助于基于Fe/ZnO界面的相关器件的设计和研发.  相似文献   

2.
王立锦  滕蛟  于广华 《物理学报》2006,55(8):4282-4286
通过分子束外延(MBE)和脉冲激光沉积(PLD)方法,将1—10个Fe原子层(ML)以楔形方式沉积到反铁磁单晶NiO(001)基片上.表面磁光克尔效应的原位测试结果表明:通过MBE沉积的Fe原子层在Fe/NiO界面处产生了约2ML的磁死层;而通过PLD沉积的Fe原子层在Fe/NiO界面处产生了约3ML的磁死层.X射线光电子能谱对Fe/NiO界面进行研究的结果表明,在Fe原子与单晶NiO间发生了界面化学反应. 关键词: 磁性薄膜 表面磁性 X射线光电子能谱  相似文献   

3.
Sb掺杂SrTio3透明导电薄膜的光电子能谱研究   总被引:2,自引:0,他引:2       下载免费PDF全文
用X射线光电子能谱和同步辐射光电子能谱研究了Sb掺杂的钙钛矿型氧化物SrTi1-xSbxO3(x=0.05,0.10,0.15,0.20)薄膜的电子结构.薄膜由紫外脉冲激光淀积在SrTiO3(001)单晶衬底上.该薄膜系列在可见光波段透明,透过率均超过90%.其导电性与掺杂浓度有关,当Sb掺杂浓度x=0.05时,薄膜显示金属型导电性.X射线光电子能谱和同步辐射光电子能谱研究结果表明,Sb掺杂在母化合物SrTiO3的禁带内引入了浅杂质能级和深杂质能级.浅杂质能级上的退局域化电子离化到导带中会产生一定的传导电 关键词: 光电子能谱 光学透过率 脉冲激光沉积薄膜  相似文献   

4.
采用X射线衍射和X射线光电子能谱实验手段对不同厚度的NiTi薄膜相变温度的变化进行了分析.结果表明在相同衬底温度和退火条件下,3?μm厚度的薄膜晶化温度高于18?μm厚度的薄膜.衬底温度越高,薄膜越易晶化,退火后薄膜奥氏体相转变温度As越低.薄膜的表面有TiO2氧化层形成,氧化层阻止了Ni原子渗出;膜与基片的界面存在Ti2O3和NiO.由于表面和界面氧化层的存在,不同厚度的薄膜内层的厚度也不同,因而薄膜越薄,Ni原子的含量就越高.Ni原子的含量的不同会影响薄膜的相变温度. 关键词: NiTi合金薄膜 X射线衍射 相变 X射线光电子能谱  相似文献   

5.
采用脉冲激光沉积技术在Si/蓝宝石衬底上制备了ZnO薄膜,结合快速退火设备研究了不同退火温度(500~900℃)及退火气氛(N2,O2)对薄膜的结构及其发光性能的影响。并优化条件得到具有最小半峰全宽及最大晶粒尺寸的薄膜。X射线衍射(XRD)结果表明:氮气氛下退火的ZnO薄膜最佳退火温度为900℃;氧气氛下退火的ZnO薄膜最佳退火温度为800℃。红外(IR)光谱中,退火后Zn-O特征振动峰红移,说明在退火过程中,原子重新排布后占据较低能量位置;同样的退火温度下,氮气氛下退火的薄膜质量更优。同步辐射光电子能谱(synchrotron-based XPS)分别表征了未退火及N2,O2下900℃退火的ZnO薄膜,分峰拟合结果表明氧气氛下退火产生更多的氧空位。结构表征结合光致发光(PL)谱表明绿光的发光峰与氧空位有关。  相似文献   

6.
本文采用X射线光电子能谱、紫外光电子能谱和低能电子衍射对室温下P在GaAs(100)表面上的生长进行了研究。结果表明,在生长初期P是成团吸附的,随着淀积量的增加而生长成α-P薄膜,该薄膜的价带结构与等离子体淀积的α-P:H薄膜的价带结构相似。在界面处有约一单层的P与衬底表面的Ga成键。α-P覆盖层使GaAs表面势垒下降约0.2eV。 关键词:  相似文献   

7.
韩亮  陈仙  杨立  王炎武  王晓艳  赵玉清 《物理学报》2011,60(6):66804-066804
利用过滤阴极真空电弧技术制备了sp3键含量不小于80%的四面体非晶碳(ta-C)膜.利用冷阴极潘宁离子源产生不同能量的氮离子对制备的ta-C薄膜进行轰击,通过X射线光电子能谱和原子力显微镜对薄膜表面结构与形貌进行分析研究.研究表明,随着氮离子的轰击能量的增大,薄膜中的CN键结构略有增大,形成了轻N掺杂;同时,在薄膜表层发生了sp3键结构向sp2键结构的转化;薄膜的表面粗糙度在经过氮离子轰击后从0.2 nm减小至0.18 nm,然后随着轰击能 关键词: 四面体非晶碳 X射线光电子能谱 摩擦系数  相似文献   

8.
硅掺杂辉光放电聚合物薄膜的热稳定性研究   总被引:1,自引:0,他引:1       下载免费PDF全文
张颖  何智兵  李萍  闫建成 《物理学报》2011,60(12):126501-126501
采用等离子体辉光放电聚合技术,在不同四甲基硅烷(TMS)流量条件下制备了硅掺杂辉光放电聚合物(Si-GDP)薄膜,采用傅里叶变换红外光谱、X射线光电子能谱和热重(TG)分析技术分析了不同TMS流量对Si-GDP薄膜结构与热稳定性的影响.结果表明:随着TMS流量在0–0.06 cm3/min范围变化,Si-GDP薄膜中Si的原子含量CSi为0–16.62%;含Si红外吸收峰的相对强度随TMS流量的增加而明显增大;Si-GDP薄膜的TG分析显示,温度在300 ℃时,随TMS流量的增加,Si-GDP薄膜的失重减少,热稳定性增强. 关键词: 硅掺杂辉光放电聚合物薄膜 X射线光电子能谱 热稳定性  相似文献   

9.
Fe/Al2O3/Fe隧道结特性分析   总被引:5,自引:0,他引:5       下载免费PDF全文
刘存业  徐庆宇  倪刚  桑海  都有为 《物理学报》2000,49(9):1897-1900
用离子束溅射方法制备磁性隧道结(MTJ). 研究MTJ样品的隧道结磁电阻(TMR)效应.用X射线 光电子能谱分析了MTJ的软、硬磁层和非磁层及其界面的化学组成与微结构.研究了MTJ的微 结构对氧化铝势垒高度与有效宽度和TMR效应的影响. 关键词: 磁性隧道结 X射线光电子能谱 隧道结磁电阻  相似文献   

10.
利用同步辐射光电子能谱研究了Fe/ZnO生长模式、界面化学反应和电子结构.结果表明,Fe在ZnO(0001)表面以类SK模式生长(单层加岛状生长).当沉积约2?的Fe后,生长模式开始从二维层状生长转变成混合模式生长.界面价带谱和Fe3p芯能级谱的分析表明,在低覆盖度下,约有一个原子层(约1.5?)的Fe被ZnO(0001)面的外层O原子氧化,随着沉积厚度的增加,金属态Fe的信号逐渐增强.当吸附了5.1?的Fe时,出现了较强的金属Fe的Fermi边,说明出现了Fe的金属态.此外,在Fe原子吸附过程中,样品功函数在Fe厚度为0.2?时达到最小值4.5eV,偶极层形成后逐渐稳定在4.9eV.  相似文献   

11.
The phase composition, electronic structure, and magnetic properties of nanostructures formed upon deposition of iron on the surface of the Si(556) vicinal face coated by a submonolayer silver film with a √3×√3-Ag structure have been studied using high-energy-resolution photoelectron spectroscopy and analysis of magnetic linear dichroism in photoemission of Fe 3p electrons. The effective thickness of the deposited iron layer is varied from 1 to 25 ?. It has been shown that a 1- to 2-? Fe coverage leads to the formation of a metastable iron silicide thin layer with a CsCl-type structure on the surface of the sample. A further deposition of Fe (up to ≈7 ?) brings about the formation of chains consisting of nonmagnetic islands of the Fe—Si solid solution on this layer, which are oriented along the steps of the substrate. A ferromagnetic alignment of the system along the surface of the sample appears only at coverages of approximately 10 ?, when larger (≈100 nm) iron islands start to grow on the solid solution layer.  相似文献   

12.
Very thin films of TiN and Ti/TiN were prepared by physical vapor deposition on iron at 500°C to investigate the phenomena occurring at the coating/substrate interface during deposition. By means of depth selective Mössbauer spectroscopy, it was found that preliminary depositions of Ti films lead to the formation of α-Fe(Ti) solid solutions. Depending on the amount of deposited Ti, the α-Ti(Fe) solid solution and Fe?Ti intermetallic compounds can form. The influence of interfacial phases on the film adhesion is discussed.  相似文献   

13.
To investigate the initial growth of Fe films on Si(0 0 1) and the Fe/Si interface, Fe films at various thicknesses have been systematically studied by soft X-ray absorption spectroscopy (XAS) and X-ray photoemission spectroscopy (XPS). The Fe L edge XAS spectrum shows a strong thickness dependence with broader line-width for thinner films. Detailed analysis of the Fe absorption signal as a function of the thickness shows that the broad linewidth of Fe L edge XAS spectra is mostly contributed by the first Fe layer at the Fe/Si interface. In contrast to XAS, Fe 2p photoemission spectra for these films are identical. However, valence band photoemission also shows a strong thickness dependence. Comparing the valence band photoemission spectra of the thin Fe/Si(0 0 1) films with that of pure Si and the thickest Fe film, the difference spectra at all thicknesses show almost identical shape indicating the same origin: the Fe/Si interface. Thus, it is mainly the first Fe layer at Fe/Si layer that is reactive with the Si substrate changing its electronic structure.  相似文献   

14.
Fe-doped ZnO film has been grown by laser molecular beam epitaxy (L-MBE) and structurally characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM), all of which reveal the high quality of the film. No secondary phase was detected. Resonant photoemission spectroscopy (RPES) with photon energies around the Fe 2p-3d absorption edge is performed to detect the electronic structure in the valence band. A strong resonant effect at a photon energy of 710 eV is observed. Fe3+ is the only valence state of Fe ions in the film and the Fe 3d electronic states are concentrated at binding energies of about 3.8 eV and 7 eV~ 8 eV. There are no electronic states related to Fe near the Fermi level. Magnetic measurements reveal a typical superparamagnetic property at room temperature. The absence of electronic states related to Fe near the Fermi level and the high quality of the film, with few defects, provide little support to ferromagnetism.  相似文献   

15.
《Current Applied Physics》2010,10(2):693-697
ZnO thin films were deposited at room temperature by pulsed laser deposition (PLD) varying the oxygen pressure. Morphological analysis using scanning electron microscope (SEM) and atomic force microscopy (AFM) demonstrated the formation of ZnO nanorods at a particular oxygen pressure. Room temperature violet luminescence was observed from these ZnO nanorods and temperature dependence of luminescence was studied. Influence of oxygen pressure on the growth of ZnO thin films by PLD was studied using the X-ray photoelectron spectroscopy of both post ablated targets and deposited films. The ZnO films were crystalline and the formation of crystalline phase is found to follow a pressure–temperature (PT) scaling with increase of temperature.  相似文献   

16.
The interplay between the phase composition, electronic structure, and magnetic properties of the Fe/Si(100)2×1 interface has been studied at the initial stages of its formation (at Fe doses up to 8 Å). The experiments were carried out in ultra high vacuum by using high-resolution photoelectron spectroscopy with synchrotron radiation. The interface magnetic properties were examined in terms of magnetic linear dichroism in angle-resolved Fe 3p core-level photoemission. It was found that at room temperature a disordered Fe–Si solid solution is formed at the first stage of Fe deposition (≤3.4 Å). In the coverage range of 3.4–4.3 Å the solid solution transforms into Fe3Si. However, the in-plane ferromagnetic ordering of the silicide occurs only at 6.8 Å Fe that demonstrates the thickness dependence of the magnetic properties of Fe3Si. The subsequent sample annealing to 150°C transforms Fe3Si to ε-FeSi, leading to the disappearance of ferromagnetic behavior.  相似文献   

17.
The interface formation between MgO dielectric layers and the atomically clean and selenium‐passivated Ge(100) surfaces has been studied using high‐resolution synchrotron radiation based photoemission spectroscopy. Atomically clean germanium was prepared by argon ion bombardment and sub‐ sequent annealing at 550 °C. MgO deposition on this surface resulted in interface oxide formation whereas no oxidation states were observed for a selenium‐treated germanium surface indicating the effectiveness of this interlayer at producing an abrupt MgO/Ge(100) interface. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

18.
We report on room temperature ferromagnetism in C-doped ZnO thin films prepared by electron beam evaporation. Magnetization, Hall effect, X-ray photoemission spectroscopy (XPS) and X-ray diffraction studies have been conducted to investigate the source and nature of ferromagnetism in C-doped ZnO. The samples were observed to have n-type conduction with the carrier concentration increasing with C doping. XPS does not give any evidence for C substituted at the O site, and is more consistent with the formation of C-O bonds and with the presence of C primarily in the +4 state. It is suggested that the ferromagnetism originates in the development of Zn vacancies that are stabilized due to the incorporation of C in a high valence state (C4+).  相似文献   

19.
ZnO:Fe薄膜制备、光学与电学性质研究   总被引:2,自引:2,他引:0  
用双靶磁控溅射设备制备了ZnO:Fe薄膜。分析了铁靶溅射功率对薄膜的光学及电学性质的影响。X射线衍射(XRD)和原子力显微镜(AFM)图像表明:ZnO:Fe薄膜为六角纤锌矿结构,且具有非常好的沿垂直于衬底的c轴择优取向。当铁靶功率小于250W时,沉积速率随铁靶功率的增加而增加。随着铁靶功率的增加,透射光谱的吸收边有微弱蓝移,透过率在可见光区超过75%。掺铁后薄膜的电阻率只有10-2Ω.cm,远小于纯氧化锌的电阻率。通过实验得到ZnO:Fe薄膜的最佳制备条件。  相似文献   

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