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1.
史力斌  李容兵  成爽  李明标 《物理学报》2009,58(9):6446-6452
采用基于密度泛函理论和平面波赝势技术的CASTEP程序对Zn1-xBexO合金电子结构和光学性质进行了计算.当0≤x≤1,其带隙从0.963 eV变化到7.293 eV.分析了晶格畸变和能带间排斥效应对带隙的影响.当Be含量x=0.125,0.25,0.375,0.5,0.625,0.75时,a/b轴压应变控制着带隙变化;当x=0.875,1时,c轴压应变控制着带隙变化.能带间的p-d排斥影响价带顶变动,Γ1vΓ1c之间排斥影响导带底变动.这些能带间的排斥效应被用来分析Zn1-xBexO带隙变动.另外,也分析了Zn1-xBexO介电函数虚部ε2. 关键词: 带结构 光学性质 应变 排斥  相似文献   

2.
A first-principles method based on density functional theory(DFT),a generalized gradient approximation(GGA),and a projector-augmented wave(PAW) are used to study the structual and band properties of wurtzite Zn1-xCdxO and Zn1-xMgxO(0 ≤x≤1) ternary alloys.By taking into account all of the possible structures,the band gaps of Zn1-xCdxO and Zn1-xMgxO alloys are corrected and compared with experimental data.  相似文献   

3.
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   

4.
在白宝石(sapphire)衬底上低温外延生长出了MgxZn1-xO晶体薄膜.x射线衍射(XRD)及能量色散x射线(EDX)分析表明,MgxZn1-xO薄膜的晶体结构依赖于薄膜中Mg的组分x,随着Mg组分的增大,MgxZn1-xO薄膜的结构从与ZnO晶体一致的六方结构转变为与MgO晶体一致的立方结构.对MgxZn1-xO薄膜的紫外透 关键词: 电子束蒸发反应 xZn1-xO晶体薄膜')" href="#">MgxZn1-xO晶体薄膜 结构和光学性能  相似文献   

5.
A.John Peter  Chang Woo Lee 《中国物理 B》2012,21(8):87302-087302
Cd1-x ZnxS nanocrystals are prepared by a co-precipitation method with different atomic fractions of Zn.The texture,structural transformation and optical properties with increasing x value in Cd1-x ZnxS are studied with scanning electron microscopy,electron diffraction patterning,and absorption spectra respectively.Quantum confinement in a strained CdS/Cd1-xZnxS related nanodot with various Zn content values is investigated theoretically.Binding energies on exciton bound CdS/CdxZn1-xS quantum dot are computed,with consideration of the internal electric field induced by the spontaneous and piezoelectric polarizations,and thereby the interband emission energy is calculated as a function of the dot radius.The optical band gap from the UV absorption spectrum is compared with the interband emission energy computed theoretically.Our results show that the average diameter of composite nanoparticles ranges from 3 nm to 6 nm.The X-ray diffraction pattern shows that all the peaks shift towards the higher diffracting angles with an increase in Zn content.The lattice constant gradually decreases as the Zn content increases.The strong absorption edge shifts towards the lower wavelength region and hence the band gap of the films increases as the Zn content increases.The values of the absorption edge are found to shift towards the shorter wave length region and hence the direct band gap energy varies from 2.5 eV for the CdS film and 3.5 eV for the ZnS film.Our numerical results are in good agreement with the experimental results.  相似文献   

6.
用射频磁控溅射法在80℃的衬底温度下制备出MgxZn1-xO(0≤x ≤030)薄膜.x射线 衍射(XRD)结果表明,MgxZn1-xO薄膜为单相六角纤锌矿结构, 没有形成任何显著 的MgO分离相,MgxZn1-xO薄膜的择优取向平行于与衬底垂直的 c轴;c轴晶格常数随着Mg含量的增加逐渐减小.在MgxZn1-xO薄膜的光透射谱中出现 锐利的吸收边,由透 射谱估算出MgxZn1-xO薄膜的带隙宽度由332eV(x=0)线性地 增加到396eV(x=030). 关键词: xZn1-xO薄膜')" href="#">MgxZn1-xO薄膜 射频磁控溅射 Mg含量  相似文献   

7.
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   

8.
An ab initio calculation based on density functional theory is applied to study the doping stability and electronic structure of wurtzite Zn1−xCdxO alloys. It is found that the different alloy configurations of Zn1−xCdxO with a given Cd content are possible thermodynamically, but having different band gaps. With increasing Cd content, the formation enthalpy of Zn1−xCdxO alloy increases sharply. The Cd-content dependence of the band-gap values can be fitted with a second-order polynomial. The reduction of band gap can be attributed to the contributions of the hybridization of Zn-4s and Cd-5s, the enhancement of p-d repulsion, and the tensile strain due to Cd-doping.  相似文献   

9.
刘强  程新路  范勇恒  杨向东 《物理学报》2009,58(4):2684-2691
采用密度泛函理论下的第一性原理平面波超软赝势方法,对Zn1-xMgxO超晶胞和掺杂Al,N后的Zn1-xMgxO超晶胞分别进行了优化计算.结合广义梯度近似计算了Al和N共掺杂后Zn1-xMgxO的能带结构、电子态密度和Mulliken电荷布居分布.计算表明:掺入N原子的2p态电子为Zn1-xMgxO价带顶提供空穴载流子,使Zn1-xMgxO价带顶向高能方向移动;掺入Al原子的3p态电子则与N原子的2p态电子在费米能级附近发生轨道杂化,使费米能级处价带能级展宽,Al和N共掺杂可获得p型Zn1-xMgxO. 关键词: 密度泛函理论 1-xMgxO')" href="#">Zn1-xMgxO 电子结构 共掺杂  相似文献   

10.
In the present computational study, we have explored the structural, electronic and optical properties of ZnTe, CdTe and HgTe binary compounds and their ternary alloys ZnxCd1-xTe, ZnxHg1-xTe and CdxHg1-xTe as well as their ordered quaternary ZnxCdyHg1-x-yTe alloys using the full potential linearized augmented plane wave (FP-LAPW) method based on the density functional theory. We have numerically estimated the total energies, the lattice parameters, the bulk moduli and their first pressure derivative using the generalized gradient approximation (GGA). The band structure is computed using the modified Becke-Johnson (TB-mBJ) approximation. Results of our study show a nonlinear dependence of the composition on the lattice constant, bulk modulus and band gap for the binary and ternary compounds as well as for the quaternary alloys. Additionally, the dielectric function, the refractive index and the loss energy were also reported. The pressure effect on the band gap energy and optical properties were also investigated and reported. Our results are in good agreement with experimental values and theoretical data available in the literature.  相似文献   

11.
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   

12.
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   

13.
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   

14.
研究了高温高压下制备MgxZn1-xO(0.30x0.60)固溶体的过程.在1000—2000℃和4—5.6GPa的条件下,制备出稳定的单一立方相MgxZn1-xO(x=0.4,0.5,0.6)固溶体,解决了常压下MgxZn1-xO的分相问题.通过X射线衍射仪和扫描电子显微镜等测试手段,对MgxZn1-xO样品进行了表征,阐明了立方相MgxZn1-xO的形成机制,给出了高压下MgxZn1-xO固溶体的温度与组分相图.  相似文献   

15.
Thin films of ternary ZnxCd1-xSe were deposited on GaAs (100) substrate using metalorganic-chemical-vapour-deposition (MOCVD) technique. Temperature dependence of the nearband-edge emission from these Cd-rich ZnxCd1-xSe (forx = 0025, 0.045) films has been studied using photoluminescence spectroscopy. Relevant parameters that describe temperature variation of the energy and broadening of the fundamental band gap have been evaluated using various models including the two-oscillator model, the Bose-Einstein model and the Varshni model. While all these models suffice to explain spectra at higher temperatures, the two-oscillator model not only explains low temperature spectra adequately but also provides additional information concerning phonon dispersion in these materials.  相似文献   

16.
采用密度泛函理论结合投影缀加波方法,对掺杂Cd导致ZnO禁带宽度下降的机理进行了研究. 通过对掺杂前后电子能带结构,态密度以及分态密度的计算和比较,发现CdxZn1-xO价带顶端(VBM)始终由O-2p占据;而导带顶端(CBM)则由Cd-5s与Zn-4s杂化轨道控制. 随着掺杂浓度的增加,决定带隙宽度的CBM的位置下降,同时VBM的位置上升,从而导致了带隙的变窄,出现了红移现象. 此外,Cd掺杂会使晶胞发生膨胀,这种张应变也是导致Cd  相似文献   

17.
Cd掺杂纤锌矿ZnO电子结构的第一性原理研究   总被引:6,自引:0,他引:6       下载免费PDF全文
采用密度泛函理论结合投影缀加波方法,对掺杂Cd导致ZnO禁带宽度下降的机理进行了研究. 通过对掺杂前后电子能带结构,态密度以及分态密度的计算和比较,发现CdxZn1-xO价带顶端(VBM)始终由O-2p占据;而导带顶端(CBM)则由Cd-5s与Zn-4s杂化轨道控制. 随着掺杂浓度的增加,决定带隙宽度的CBM的位置下降,同时VBM的位置上升,从而导致了带隙的变窄,出现了红移现象. 此外,Cd掺杂会使晶胞发生膨胀,这种张应变也是导致Cd 关键词: 密度泛函理论 电子结构 Cd掺杂ZnO  相似文献   

18.
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   

19.
This paper reports that Al1 xInxN epilayers were grown on GaN template by metalorganic chemical vapor de-position with an In content of 7%-20%. X-ray diffraction results indicate that all these Al1 xInxN epilayers have a relatively low density of threading dislocations. Rutherford backscattering/channeling measurements provide the exact compositional information and show that a gradual variation in composition of the Al1 xInxN epilayer happens along the growth direction. The experimental results of optical reflection clearly show the bandgap energies of Al1 xInxN epilayers. A bowing parameter of 6.5 eV is obtained from the compositional dependence of the energy gap. The cathodoluminescence peak energy of the Al1 xInxN epilayer is much lower than its bandgap, indicating a relatively large Stokes shift in the Al1 xInxN sample.  相似文献   

20.
In this paper, we present a theoretical study of the quantized electronic states in Cd1-xZnxS quantum dots. The shape of the confining potential, the subband energies and their eigen envelope wave functions are calculated by solving a one-dimensional Schr?dinger equation. Electrons and holes are assumed to be confined in dots having a flattened cylindrical geometry with a finite barrier height at the boundary. Optical absorption measurements are used to fit the bandgap edge of the Cd1-xZnxS nanocrystals. An analysis of the electron band parameters has been made as a function of Zn composition. Two main features were revealed: (i) a multiplicity in Cd1-xZnxS quantum dots with different crystalline sizes has been found to fit accurately experimental data in the composition range 0 ≤x ≤0.2; (ii) the fit did not, however, show a multiplicity for x higher than 0.4. On the other hand, we have calculated the energy level structure of coupled Cd1-xZnxS semiconductor quantum dots using the tight-binding approximation. As is found the Zn composition x = 0.4 is expected to be the most favorable to give rise a superlattice behavior for the Cd1-xZnxS quantum dots studied.  相似文献   

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