Calculation of electronic and optical properties of zinc blende GaP1 − xNx

In order to clarify the electronic properties of the ternary compound semiconductor GaPN, in a zinc-blende structure, a simple pseudopotential scheme (EPM), within an effective potential (VCA), is proposed. The effects of disorder and spin–orbit coupling are neglected. Various quantities, such as energy levels, charge densities, ionicity character, transverse effective charge, and refractive index are obtained for this alloy. Moreover, the crossover of the direct and indirect band gaps is predicted.     

基于自洽GW方法的碳化硅准粒子能带结构计算

在多体微扰理论的框架下, 分别采用G₀W₀方法和准粒子自洽GW方法计算3C-SiC和2H-SiC的准粒子能级. 由一个平均Monkhorst-Pack网格点上的准粒子能级和准粒子波函数出发, 结合最局域Wannier函数插值, 得到3C-SiC和2H-SiC的自洽准粒子能带结构. 3C-SiC的价带顶在Γ点, 导带底在X点. DFT-LDA, G₀W₀和准粒子自洽GW给出的3C-SiC间接禁带宽度分别为 1.30 eV, 2.23 eV和2.88 eV. 2H-SiC价带顶在Γ 点, 导带底在K点. 采用DFT-LDA, G₀W₀和准粒子自洽GW方法得到的间接禁带宽度分别为2.12 eV, 3.12 eV和 3.75 eV. 计算基于赝势方法, 对于3C-SiC和2H-SiC的准粒子自洽GW计算给出的禁带宽度均比实验值略大.     

Wavelength modulation spectra of SbSI and its electronic band structure

The reflectivities of SbSI and their logarithmic derivatives between 1.8 and 4.5 eV have been measured at different temperatures. The structures in the reflectivities are compared with those calculated independently by the empirical pseudopotential method (EPM), using the pseudopotential form factors scaled from previous band structure calculations of other crystals. The large optical anisotropy of SbSI is explained. A preliminary band structure for SbSI is presented.     

Pseudopotential study of bonding and ionicity in InP at various pressures

We have investigated the chemical trends of the III–V semiconductor InP in the zinc-blende structure under hydrostatic pressure by means of empirical pseudopotential calculations. The pressure coefficients of the main band gaps (at Γ, X, and L) are given and compared with the available experimental data. In agreement with experiments, we find that the transverse effective charge decreases with increasing pressure which indicates the increased covalent bonding in the studied material.     

Band structure and electronic properties of InP

A combination of the pseudopotential method with thek,p method was used to calculate the complete band structure of InP. The pseudopotential form factors were determined by fitting to conduction band energy spacings, optical spectra, and density of states properties. Effective masses for important conduction band minima and pressure coefficients for some transiton energies were evaluated and compared with experimental data as far as possible.     

sp3sTight-binding parameters for transport simulations in compound semiconductors

A genetic algorithm approach is used to fit orbital interaction energies of sp3s* tight-binding models for the nine binary compound semiconductors consistent of Ga, Al, In and As, P, Sb at room temperature. The new parameters are optimized to reproduce the bandstructure relevant to carrier transport in the lowest conduction band and the highest three valence bands. The accuracy of the other bands is sacrificed for the better reproduction of the effective masses in the bands of interest. Relevant band edges are reproduced to within a few meV and the effective masses deviate from the experimental values typically by less than 10%.     

Electronic and optical properties of SbSBr,SbSI and SbSeI

Band structures of SbSBr and SbSeI have been obtained by using the empirical pseudopotential method (EPM) to fit our measured optical reflectivity data and earlier gap measurements. An SbSI band structure has been determined by fitting to earlier reflectivity and Raman spectroscopic data, and the results agree better with the data than do the results of an earlier preliminary EPM calculation. Secondary conduction band minima may in part be responsible for the observed microwave oscillation (Gunn effect) in SbSI. Similar minima in SbSBr and SbSeI are reported, suggesting these crystals might also show microwave properties. The total densities of states are presented.     

Phonon and Polaron properties in InSb spherical quantum dots

The size-dependent energy gaps, electron and heavy hole effective masses, phonon frequencies and polaron related parameters in InSb spherical quantum dots are investigated. The calculations are performed using a pseudopotential approach. Good agreement is obtained between our results and those of the literature for bulk InSb. When proceeding from bulk to nano-scale, all studied properties are found to be changed significantly. This is attributed to the quantum confinement effect.     

Electronic and optical properties of InSb quantum dots from pseudopotential calculation

The electronic and optical features of InSb spherical quantum dots have been investigated by a pseudopotential approach as a function of their radius taken in the range 1-10 nm. The direct- and indirect band gaps along with the electron and heavy hole effective masses are all found to be diminished as the quantum dot radius is increased. However, the refractive index, the static- and high frequency dielectric constant as well as the transverse effective charge are shown to be augmented by increasing the quantum dot radius. It is noted that the quantum confinement is of great impact on all the studied quantities for quantum dot radius below 6 nm. This could result in more opportunities to obtain desired optoelectronic properties that cannot be obtained in the bulk InSb materials.     

Electronic structure of transparent oxides with the Tran-Blaha modified Becke-Johnson potential

We present electronic band structures of transparent oxides calculated using the Tran-Blaha modified Becke-Johnson (TB-mBJ) potential. We studied the basic n-type conducting binary oxides In(2)O(3), ZnO, CdO and SnO(2) along with the p-type conducting ternary oxides delafossite CuXO(2) (X=Al, Ga, In) and spinel ZnX(2)O(4) (X=Co, Rh, Ir). The results are presented for calculated band gaps and effective electron masses. We discuss the improvements in the band gap determination using TB-mBJ compared to the standard generalized gradient approximation (GGA) in density functional theory (DFT) and also compare the electronic band structure with available results from the quasiparticle GW method. It is shown that the calculated band gaps compare well with the experimental and GW results, although the electron effective mass is generally overestimated.     

强激光照射对6H-SiC晶体电子特性的影响

使用基于密度泛函微扰理论的第一性原理赝势法, 模拟研究了纤锌矿6H-SiC晶体在强激光照射下电子特性的变化. 研究结果表明, 电子温度T_e在升高到3.89 eV及以上后, 6H-SiC由间接带隙的晶体变为直接带隙的晶体; 带隙值随电子温度T_e升高先是增大后又快速减小, 当电子温度T_e大于4.25 eV以后, 带隙已经消失而呈现出金属特性.     

SiC多型体几何结构与电子结构研究

采用平面波超软赝势法和范数不变赝势法对几种SiC多型体的几何结构、能带结构等进行了系统的研究.结果表明:6HSiC导带最低点在ML线上U点,用平面波超软赝势法计算时U点在(0000,0500,0176)点附近;而用范数不变赝势法计算时在导带最低点附近能带呈现不连续点,不连续点出现在(0000,0500,0178)点附近.两种赝势法计算结果相比,用平面波超软赝势法得到的导带最低点位置更靠近布里渊区M(0,05,0)点.在平面波超软赝势下,随着六角度的增加,cp,cpa增大的趋势较为明显,能隙和价带宽度变宽的趋势也较为明显.在计算极限内,绝对零度下4HSiC系统能量最低、最稳定,而Ewald能量显示3CSiC最稳定. 关键词： 密度泛函理论 电子结构 SiC     

二维6H-SiC光学特性的应变调控

为了减小6H-SiC的带隙、提高对可见光的吸收效率和载流子迁移速率，采用第一性原理研究了应变对6H-SiC的能带结构、光学吸收系数、载流子迁移率以及光催化特性的影响。结果表明：应变能够降低6H-SiC的导带底，但对价带顶没有影响，导致带隙减小。随着应变的增加，吸收曲线向低能级方向移动，即发生红移，有利于可见光的吸收。施加应变后空穴的载流子迁移率提高，有利于载流子移动，且空穴的载流子迁移率是电子的2.5倍，有利于空穴和电子的分离。综合应变对带隙大小、带边位置的影响可知，应变在±2%、±4%时对可见光的吸收以及光催化制氢最有效。综上所述，应变能够对6H-SiC的光学吸收和光催化特性有很好的调控作用。     

Electrical resistivity of the Ti\mathsf{_4}O\mathsf{_7} Magneli phase under high pressure

The electronic and positronic properties of the pentanary semiconductor alloys Ga_xIn_1-xP_ySb_zAs_1-y-z lattice matched to GaSb have been studied. The electron wave function is calculated semiempirically using the pseudopotential band model under the virtual crystal approximation. The positron wave function is evaluated under the point core approximation for the ionic potential. Electronic and positronic quantities namely, electronic structure and band gaps, positron band structure, effective mass and affinity, and electron-positron momentum densities have been predicted and their dependence on the phosphorus composition has been discussed. Received 30 August 2002 / Received in final form 12 February 2003 Published online 24 April 2003     

Electronic structure and optical properties of CdSexTe1−x mixed crystals

The band structure and optical properties of the CdSe_xTe_1−x ternary mixed crystals have been studied using the pseudopotential formalism under an improved virtual crystal approximation approach. Quantities such as, energy gaps, band-gap bowing parameters, electron effective mass and dielectric constants are calculated. Our results agree well with the available data in the literature. The composition dependence of all studied quantities has been expressed by quadratic polynomial forms.     

First-principles Band Structures Calculation of Tin-phthalocyanine

SnPc(Tin-phthalocyanine)因在无机/有机二极管等光电结构器件中表现出了很多有趣的特性而备受关注.为了更深地理解载流子的传输特性,利用密度泛函理论,采用广义梯度近似(DFT-GGA),关联函数选择BLYP计算了SnPc的能带结构.从点波函数、能带带宽以及带隙分析了载流子的传输行为. 从前线轨道的带宽以及电子和空穴的有效质量,可以看到电子的传输要比空穴的传输容易两倍左右.而且,当研究费米能级附近的能带时,发现未占有带的带隙总体上要小于占有带的带隙,这表明在考虑声子参与的情况下,电子在带间的跳跃要比空穴容易得多.以上的事实说明SnPc是一种电子传输占主导的材料.     

Electronic structure of collapsed C,BN, and BC3 nanotubes

The electrical properties of single-wall C, BN, and BC₃ nanotubes in ideally rolled-up forms show a wide spectrum from truly metals to large band gap semiconductors. In the presence of radial deformations that collapse tubes, the electrical properties are severely modified such that metals turn into semiconductors and vice versa. Based on first-principles pseudopotential calculations, we find that metallic C nanotubes have a finite band gap if radial deformations break all mirror symmetries of the tubes, and that original finite gaps (∼0.5 eV) of semiconducting C and BC₃ tubes are closed by collapsing deformations. In BN tubes, band gaps can be tuned in the range 2–5 eV. On the other hand, the band gaps of armchair BN and zigzag BC₃ nanotubes are found to be insensitive to radial deformations. These new findings can be applied to design new types of nanotube-based functional devices using radial deformations.     

Band structure of AlSb

A combination of the pseudopotential method with thek. p method was used to calculate the complete band structure of AlSb. The pseudopotential form factors were determined by fitting to reliably assigned optical transition energies. Optical critical points and effective masses were evaluated and compared with experimental data so far as possible.This work was performed in the Arbeitsgemeinschaft A_IIIB_V-Halbleiter of the Karl-Marx University Leipzig. The authors are indebted to Dr. K.Unger for stimulating discussions.     

Charge density of Ga<Subscript><Emphasis Type="Italic">x</Emphasis></Subscript>Al<Subscript>1 − <Emphasis Type="Italic">x</Emphasis></Subscript>Sb

Charge density calculations and electronic band structures for Ga _x Al_{1 − x} Sb with x = 1.0, 0.5 and 0.0 are presented in this work. The calculations are performed using the empirical pseudopotential method. The charge density is computed for a number of planes, i.e. z = 0.0, 0.125 and 0.25 A ₀ by generating the potential through a number of potential parameters available in the literature. The virtual crystal approximation was applied for the semiconducting alloy. The characteristics of the band structure and charge density are observed to be affected by the potential parameters. Calculated band gaps and the nature of gaps are in good agreement with the experimental data reported. The ionicity is also reasonably in good agreement with other scales proposed in the literature; however the formulation needs to be improved. The present work also demands indirect experimental band gap for the alloy.      

Empirical pseudo-potential calculation of the in-plane effective masses of electron and holes of two-dimensional excitons in CdTe quantum wells

The electron and hole effective masses associated with the in-plane motion of an exciton in a quantum well are often derived from the Luttinger parameters associated with the bulk band structure. In this work empirical pseudo-potential calculations of the bulk band structure of CdTe including spin-orbit coupling are presented. For an exciton, mapping the real space in-plane motion of the electron and hole on tok-space allows the effective masses to be calculated from the pseudo-potential band structure at all points around the exciton orbit. The calculations reveal that for CdTe the in-plane masses of the electron, light- and heavy-hole are similar to those commonly accepted for motion along the growth orz-axis, i.e. 0.11, 0.15 and 0.45, respectively. The implications of these effective masses for exciton binding energies are discussed.