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1.
采用脉冲激光沉积(PLD)方法在单晶Si(100)衬底上沿c轴方向生长单晶Zn1-xMgxO薄膜,通过X射线衍射(XRD)、原子力显微镜(AFM)、扫描电镜(SEM)和荧光光谱(PL)研究了膜厚、Mg含量、退火温度及氧气氛等制备工艺对Zn1-xMgxO薄膜的结构、形貌和光学性质的影响.实验结果表明,Mg含量x≤0.15时, Zn关键词: 1-xMgxO薄膜')" href="#">Zn1-xMgxO薄膜 制备工艺 结构 光学性质  相似文献   

2.
郑树文*  范广涵  张涛  苏晨  宋晶晶  丁彬彬 《物理学报》2013,62(3):37102-037102
采用密度泛函理论框架下的第一性原理平面波超软赝势方法, 对纤锌矿BexZn1-xO合金进行能隙特性、弯曲系数和结构参数的计算. 结果表明: BexZn1-xO合金的能隙和弯曲系数都随Be掺杂组分的增大而增大. 通过修正BexZn1-xO合金的能隙值得知其合金弯曲系数b为6.02 eV, 这与实验值接近. 纤锌矿BexZn1-xO合金的能隙弯曲系数过大主要来源于体积形变和电荷转移的贡献. 文中还分析了BexZn1-xO合金的晶格常数、 平均键长和平均次近邻原子距离与Be组分的关系.  相似文献   

3.
利用X射线吸收精细结构、X射线衍射和磁性测量等技术研究脉冲激光气相沉积法制备的Zn1-xCoxO (x=0.01,0.02)稀磁半导体薄膜的结构和磁性.磁性测量结果表明Zn1-xCoxO样品都具有室温铁磁性.X射线衍射结果显示其薄膜样品具有结晶良好的纤锌矿结构.荧光X射线吸收精细结构测试结果表明,脉冲激光气相沉积法制备的样品中的Co离子全部进入ZnO晶格中替代了部分Zn的格点位置,生成单一相的Zn1-xCoxO 稀磁半导体.通过对X射线吸收近边结构谱的分析,确定Zn1-xCoxO薄膜中存在O空位,表明Co离子与O空位的相互作用是诱导Zn1-xCoxO产生室温铁磁性的主要原因. 关键词: 1-xCoxO稀磁半导体')" href="#">Zn1-xCoxO稀磁半导体 X射线吸收精细结构谱 脉冲激光气相沉积法  相似文献   

4.
吕兵  周勋  令狐荣锋  王晓璐  杨向东 《中国物理 B》2011,20(3):36104-036104
This paper carries out first principles calculation of the structure,electronic and optical properties of Be x Zn 1 x O alloys based on the density-functional theory for the compositions x = 0.0,0.25,0.5,0.75,1.0.The lattice constants deviations of alloys obey Vegard’s law well.The Be x Zn 1 x O alloys have the direct band gap(Γ-Γ) character,and the bowing coefficients are less than the available theoretical values.Moreover,it investigates in detail the optical properties(dielectric functions,absorption spectrum and refractive index) of these ternary mixed crystals.The obtained results agree well with the available theoretical and experimental values.  相似文献   

5.
Ge1-xSnx是一种新型IV族合金材料, 在光子学和微电子学器件研制中具有重要应用前景. 本文使用低温分子束外延(MBE)法, 在Ge(001)衬底上生长高质量的Ge1-xSnx合金, 组分x分别为1.5%, 2.4%, 2.8%, 5.3%和14%, 采用高分辨X射线衍射(HR-XRD)、卢瑟福背散射谱(RBS) 和透射电子显微镜(TEM)等方法表征Ge1-xSnx合金的材料质量. 对于低Sn组分(x≤ 5.3%)的样品, Ge1-xSnx合金的晶体质量非常好, RBS的沟道/随机产额比(χmin)只有5.0%, HR-XRD曲线中Ge1-xSnx衍射峰的半高全宽(FWHM)仅100' 左右. 对于x=14%的样品, Ge1-xSnx合金的晶体质量相对差一些, FWHM=264.6'. 关键词: 锗锡合金 锗 分子束外延  相似文献   

6.
郑树文  范广涵  何苗  姚光锐  陈峻  贺龙飞 《物理学报》2012,61(17):177102-177102
采用基于密度泛函理论平面波赝势方法, 对纤锌矿BeO掺Cd的Be1-xCdxO合金进行电子结构与能带特性研究. 结果表明: Be1-xCdxO的价带顶始终由O 2p电子态决定, 而导带底由Be 2s和Cd 5s的电子态决定.随着Be1-xCdxO合金的Cd掺杂量增加, Cd 4d与O 2p的排斥效应逐渐加强, 同时Be1-xCdxO的带隙逐渐变小, 出现"直接-间接-直接"的带隙转变. 为了使理论值与实验值相一致, 对Be1-xCdxO带隙进行修正, 并分析了纤锌矿BeO-ZnO-CdO三元合金的带隙和弯曲系数与晶格常数的关系.  相似文献   

7.
Structural, electronic and optical properties as well as structural phase transitions of ternary alloy CdxZn1 − xS have been investigated using the first-principles calculations based on the density functional theory. We found that the crystal structure of CdxZn1 − xS alloys transforms from wurtzite to zinc blende as Cd content of x=0.83x=0.83. Effect of Cd content on electronic structures of CdxZn1 − xS alloys has been studied. The bandgaps of CdxZn1 − xS alloys with wurtzite and zinc blende structures decrease with the increase of Cd content. Furthermore, dielectric constant and absorption coefficient also have been discussed in detail.  相似文献   

8.
Ba(Ti1−x,Nix)O3 thin films were prepared on fused quartz substrates by a sol–gel process. X-ray diffraction and Raman scattering measurements showed that the films are of pseudo-cubic perovskite structure with random orientation and the change of lattice constant caused by Ni-doping with different concentrations is very small. Optical transmittance spectra indicated that Ni-doping has an obvious effect on the energy band structure. The energy gap of Ba(Ti1−x,Nix)O3 decreased linearly with the increase of Ni concentration. It indicates that the adjusting of band gap can be achieved by controlling the Ni-doping content accurately in Ba(Ti1−x,Nix)O3 thin films. This has potential application in devices based on ferroelectric thin films.  相似文献   

9.
The structural, electronic and thermodynamic properties of the SrS1–xOx ternary mixed crystals have been studied using the ab initio full potential linearized augmented plane wave (FP-LAPW) method within density functional theory. The effect of composition on lattice parameter, bulk modulus and band gap was investigated. The lattice constants from Vegard's law and the bulk modulus from linear concentration dependence were observed for the alloys. The microscopic origins of the gap bowing were explained by using the approach of Zunger and co-workers. The thermodynamic stability of these alloys was investigated by calculating the excess enthalpy of mixing ΔHm as well as the phase diagram. In addition to FP-LAPW method, the composition dependence of the refractive index and the dielectric constant was studied by different models.  相似文献   

10.
Thin films of amorphous Se100−xSbx (x=5,10 and 20 at%) system are deposited on a silicon substrate at room temperature (300 K) by thermal evaporation technique. The optical constant such as refractive index (n) has been determined by a method based on the envelope curves of the optical transmission spectrum at normal incidence by a Swanpoel method. The oscillator energy (Eo), dispersion energy (Ed) and other parameters have been determined by the Wemple–DiDomenico method. The absorption coefficient (α) has been determined from the reflectivity and transmitivity spectrum in the range 300–2500 nm. The optical-absorption data indicate that the absorption mechanism is a non-direct transition. We found that the optical band gap, Egopt, decreases from 1.66±0.01 to 1.35±0.01 eV with increase Sb content.  相似文献   

11.
利用X射线衍射(XRD)和X射线吸收近边结构(XANES)方法研究了在Si(100)衬底上及600℃温度条件下用分子束外延(MBE)共蒸发方法生长的MnxSi1-x磁性薄膜的结构.由XRD结果表明,只有在高Mn含量(8%和17%)样品中存在着Mn4Si7化合物物相.而XANES结果则显示,对于Mn浓度在0.7%到17%之间的MnxSi1-x样品,其Mn原子的XANES谱表现出了一致的谱线特征.基于多重散射的XANES理论计算进一步表明,只有根据Mn4Si7模型计算出的理论XANES谱才能够很好的重构出MnxSi1-x样品的实验XANES谱.这些研究结果说明在MnxSi1-x样品中,Mn原子主要是以镶嵌式的Mn4Si7化合物纳米晶颗粒存在于Si薄膜介质中,几乎不存在间隙位和替代位的Mn原子. 关键词xSi1-x磁性薄膜')" href="#">MnxSi1-x磁性薄膜 分子束外延 XRD XANES  相似文献   

12.
成功生长了Co50Ni21Ga29:Si(x=1,2)单晶样品,对其磁性,马氏体相变及其相关性质进行了细致的测量.发现掺Si成分的单晶具有非常迅速的马氏体相变行为、2.5%的大相变应变、大于100 ppm的磁感生应变和4.5%的相变电阻.进一步研究指出,在CoNiGa合金中掺入适量Si元素,能够降低材料的马氏体相变温度,减小相变热滞后,提高材料的居里温度,并使得磁性原子的磁矩有所降低.尤其重要的是Si元素的添加能够增大材料马氏体的磁晶各向异性能,改善马氏体变体的迁移特性,从而获得更大的磁感生应变. 关键词: 铁磁形状记忆合金 Heusler合金 50Ni21Ga29Six')" href="#">Co50Ni21Ga29Six  相似文献   

13.
针对Co(S1-xSex)2系统在x=0.11附近发生的铁磁金属到顺磁金属相变,制备了一系列不同Se替代浓度的多晶样品.通过对其结构和电阻率-温度ρ(T)关系的系统观测,结果发现,样品铁磁相变温度TC随着Se替代浓度x值的增加,以(1-x)1/2关系单调下降,其二级铁磁相变转变为一级相变 关键词: 量子相变 自旋量子涨落 1-xSex)2')" href="#">Co(S1-xSex)2  相似文献   

14.
针对NiS2-xSex系统在x=1.00附近发生的反铁磁量子相变,制备了一系列NiS2-xSex(x=0.96, 0.98, 1.00, 1.05, 1.10和1.20)多晶样品,对其结构、磁性质和电阻率进行了系统的观测.结果发现:样品磁化率-温度关系呈现典型的强关联电子系统特征;与铜氧化物超导体相类似,它们的电阻率-温度关系在很宽的温 关键词: 量子相变 反铁磁自旋涨落 2-xSex体系')" href="#">NiS2-xSex体系  相似文献   

15.
利用脉冲激光沉积方法制备出了具有室温铁磁性的Ni1-xFexO(x=0.02,0.05)稀磁半导体.X射线衍射(XRD)结果表明Ni1-xFexO的晶体结构为NaCl结构,并且在Fe含量较高的Ni0.95Fe0.05O中出现了少量的α-Fe2O3物相.X射线吸收近 关键词: 1-xFexO')" href="#">Ni1-xFexO XANES 脉冲激光沉积方法  相似文献   

16.
MgxZn1-xO thin films have been prepared on silicon substrates by radio frequency magnetron sputtering at 60℃. The thin films have hexagonal wurtzite single-phase structure and a preferred orientation with the c-axis perpendicular to the substrates. The refractive indices of MgxZn1-xO films are studied at room temperature by spectroscopic ellipsometry over the wavelength range of 400--760\,nm at the incident angle of 70℃. Both absorption coefficients and optical band gaps of MgxZn1-xO films are determined by the transmittance spectra. While Mg content is increasing, the absorption edges of MgxZn1-xO films shift to higher energies and band gaps linearly increase from 3.24.eV at x=0 to 3.90\,eV at x=0.30. These results provide important information for the design and modelling of ZnO/ MgxZn1-xO heterostructure optoelectronic devices.  相似文献   

17.
高华  高大强  薛德胜 《中国物理 B》2011,20(5):57502-057502
The Fe100-xMox(13≤x≤25) alloy nanowire arrays are synthesized by electrodeposition of Fe 2+ and Mo 2+ with different ionic ratios into the anodic aluminum oxide templates.The crystals of Fe100-xMox alloy nanowires gradually change from polycrystalline phase to amorphous phase with the increase of the Mo content and the nanowires are of amorphous structure when the Mo content reaches 25 at%,which are revealed by the X-ray diffraction and the selected area electron diffraction patterns.As the Mo content increases,the magnetic hysteresis loops of Fe100-xMox alloy nanowires in parallel to the nanowire axis are not rectangular and the slopes of magnetic hysteresis loops increase.Those results indicate that the magnetostatic interactions between nanowires and the magnetocrystalline anisotropy both have significant influences on the magnetization reversal process of the nanowire arrays.  相似文献   

18.
利用固相反应烧结技术制备La0.1Bi0.9-xEuxFeO3系列化合物. 利用X射线粉末衍射进行物相鉴定和结构分析,确定了材料的相关系:x≤0.05,材料为R3c结构相;0.08≤x≤0.12,材料为赝R3c结构相;x≥0.15是Pbnm相,其中0.15≤x≤0.20区域Pbnm相存在畸变. 磁测量结果表明,材料具有弱铁磁性,对于x≤0.20材料,磁矩在x=0.12成分存在极值. 利用阻抗分析仪测量了室温介电常数随成分的变化关系.讨论了材料的结构与弱铁磁性和室温介电常数间的关系. 关键词: 0.1Bi0.9-xEuxFeO3')" href="#">La0.1Bi0.9-xEuxFeO3 X射线衍射 磁性 介电常数  相似文献   

19.
The vapor grown SbSBrxI1−x (x=0.1; 0.5; 0.9) crystals with clear mirror surfaces have been used for infrared reflection measurements with Fourier spectrometer. The vibration frequencies along c(z)-axis have been derived from Kramers–Kroning and optical parameters fitting analysis of the experimental reflectivity spectra at T=300 K. The theoretical vibration spectra of SbSBrxS1−x (x=0.1; 0.5; 0.9) crystals in paraelectric phase (T=300 K) along c(z)-axis have been determined in quasiharmonic approximation by diagonalization of dynamical matrix. The theoretical vibration spectra of these crystals in ab(xy) plane have been determined in harmonic approximation. In this work we discuss the nature of anharmonism in SbSBrxI1−x crystals along the c(z)-axis.  相似文献   

20.
Using density-functional calculations, we investigate the special properties of SrFe1−xCoxO3. The results show that the ground states have A-type antiferromagnetic order for x=0.1 and ferromagnetic order for x≥0.2 with Co ions distributed averagely. SrFe1−xCoxO3 exhibits half-metallic nature for 0.2≤x≤0.7 and full-metallic nature for other values of x, and the half-metallic gap decreases with increasing x. The tunneling between the half-metallic ferromagnetic phases drives the large magnetoresistance. In addition, the Co cations are in the intermediate-spin state, while the Fe cations are in the intermediate-spin state for x≤0.5 and the high-spin state for x≥0.6.  相似文献   

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