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1.
采用第一性原理贋势平面波方法对(110)应变下立方相Ca2P0.25Si0.75的能带结构及光学性质进行模拟计算,全面分析了应变对Ca2P0.25Si0.75能带结构、光学性质的影响。计算结果表明:在92%~100%压应变范围内随着应变的逐渐增大导带向低能方向移动,价带向高能方向移动,带隙呈线性逐渐减小,但始终为直接带隙;在100%~102%张应变范围内随着应变的增加,带隙呈逐渐增大,应变达到102%直接带隙最大Eg=0.54378eV;在102%~104%应变范围内随着应变的增加,带隙逐渐减小;当应变大于104%带隙变为间接带隙且带隙随着应变增大而减小。施加应变Ca2P0.25Si0.75的介电常数、折射率均增大;施加压应变吸收系数增加,反射率减小;施加张应变吸收系数减小,反射率增加。综上所述,应变可以改变Ca2P0.25Si0.75的电子结构和光学常数,是调节Ca2P0.25Si0.75光电传输性能的有效手段。  相似文献   

2.
采用第一性原理贋势平面波方法对(110)应变下立方相Ca_2P_(0.25)Si_(0.75)的能带结构及光学性质进行模拟计算,全面分析了应变对Ca_2P_(0.25)Si_(0.75)能带结构、光学性质的影响.计算结果表明:在92%~100%压应变范围内随着应变的逐渐增大导带向低能方向移动,价带向高能方向移动,带隙呈线性逐渐减小,但始终为直接带隙;在100%~102%张应变范围内随着应变的增加,带隙呈逐渐增大,应变达到102%直接带隙最大Eg=0.54378 e V;在102%~104%应变范围内随着应变的增加,带隙逐渐减小;当应变大于104%带隙变为间接带隙且带隙随着应变增大而减小.施加应变Ca_2P_(0.25)Si_(0.75)的介电常数、折射率均增大;施加压应变吸收系数增加,反射率减小;施加张应变吸收系数减小,反射率增加.综上所述,应变可以改变Ca_2P_(0.25)Si_(0.75)的电子结构和光学常数,是调节Ca_2P_(0.25)Si_(0.75)光电传输性能的有效手段.  相似文献   

3.
采用基于密度泛函理论的第一性原理方法,在局域密度近似(LDA)下研究了B掺杂Si/SiO_2界面及其在压强作用下的电子结构和光学性质.能带的计算结果表明:掺杂前后Si/SiO_2界面均属于直隙半导体材料,但掺B后界面带隙由0. 74 eV减小为0. 57 eV,说明掺B使材料的金属性增强;对B掺杂Si/SiO_2界面施加正压强,发现随着压强不断增大,Si/SiO_2界面的带隙呈现了逐渐减小的趋势,并且由直隙逐渐转变为间隙.光学性质的计算结果表明:掺B对Si/SiO_2界面在低能区(即红外区)的介电函数虚部、吸收系数、折射率以及反射率等光学参数有显著影响,且在红外区出现新的吸收峰;对B掺杂Si/SiO_2界面施加正压强,随着压强增大,红外区的吸收峰逐渐消失,而在紫外区出现了吸收峰.上述结果表明,对Si/SiO_2界面掺B及施加正压强均可调控Si/SiO_2界面的电子结构与光学性质.本文的研究为基于Si/SiO_2界面的光电器件研究与设计提供一定的理论参考.  相似文献   

4.
采用密度泛函理论框架下的第一性原理平面波赝势方法,计算单轴应变下闪锌矿氮化铟的电子结构及光学性质.结果表明:施加应变会使带隙变窄.对于拉应变,随着应变增大带隙减小程度增大;对于压应变,随应变增大带隙减小程度减弱;且拉、压应变对带隙调控都是线性的.在能量区间4 eV~12 eV范围内施加应变时,氮化铟的吸收光谱发生红移,随拉应变程度增加,吸收光谱的红移进一步加大;随压应变增加,吸收光谱红移减弱;在该范围内,氮化铟的折射率、反射率随拉应变的增大而增加,随压应变增加减小;施加拉应变时能量损失函数峰值增大,施加压应变后能量损失函数峰值减小.通过施加单轴应变能有效调节氮化铟材料的电结构及光学性质.  相似文献   

5.
基于密度泛函理论体系下的广义梯度近似,本文利用第一性原理方法着重研究了[112]晶向硅锗异质结纳米线的电子结构与光学性质.能带结构计算表明:随着锗原子数的增加,[112]晶向硅锗纳米线的带隙逐渐减小;对Si_(36)Ge_(24)H_(32)纳米线施加单轴应变,其能量带隙随拉应变的增加而单调减小.光学性质计算则表明:随着锗原子数的增加,[112]硅锗纳米线介电函数的峰位和吸收谱的吸收边均向低能量区移动;而随着拉应变的增大,吸收系数峰值呈现出逐渐减小的趋势,且峰位不断向低能量区移动,上述结果说明锗原子数的增加与施加拉应变均导致[112]硅锗纳米线的吸收谱产生红移.本文的研究为硅锗异质结纳米线光电器件研究与设计提供一定的理论参考.  相似文献   

6.
使用第一性原理密度泛函理论(DFT)框架下的广义梯度近似(GGA+U)方法计算单轴应变对纤锌矿结构GaN的键长、差分电荷密度、电子结构以及光学性质的影响.结果表明:带隙随应变的增加而减小,压应变在(-1%~-3%)范围内变化时带隙变化不明显,压应变超过3%时带隙随应变的增大显著减小.光学性质研究表明,应变对介电函数虚部峰的位置和大小都产生影响,静态介电常数随应变的增大而增大;应变使GaN的吸收系数减小.  相似文献   

7.
采用基于第一性原理的密度泛函理论(DFT)赝势平面波方法,对块体及掺Sc的正交相Ca2Si的电子结构和光学性质进行了系统计算.计算结果表明,掺Sc后的Ca2Si能带向低能端偏移,形成n型半导体,正交相结构能隙变为0.6084eV,相比块体Ca2Si带隙加宽了一倍,但仍为直接带隙半导体.Ca2Si掺杂Sc后,正交相导带主要是Ca的4s、3d态和Sc的3d、3p态电子构成,静态介电常数变大,折射率也变大,吸收系数相比块体在低能段基本无变化,在高能段虽吸收系数减小,但仍保持105数量级且大于β-FeSi2的吸收系数,说明Ca2Si在太阳能电池上具有较好的应用前景.通过掺杂有效调制了Ca2Si的电子结构和光学性质,计算结果为Ca2Si光电材料的设计与应用提供了理论依据.  相似文献   

8.
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。  相似文献   

9.
采用基于密度泛函理论的平面波超软赝势方法,在局域密度近似(LDA)下研究了Si纳米层厚度和O空位缺陷对Si/SiO2界面电子结构及光学性质的影响.电子结构计算结果表明:在0.815~2.580nm的Si层厚度范围内,Si/SiO2界面结构的能隙随着厚度减小而逐渐增大,表现出明显的量子尺寸效应,这与实验以及其他理论计算结果一致;三种不同的O空位缺陷的存在均使得Si/SiO2界面能隙中出现了缺陷态,费米能级向高能量方向移动,且带隙有微弱增加.光学性质计算结果表明:随着Si纳米层厚度的减小,Si/SiO2界面吸收系数产生了蓝移;O空位缺陷引入后,界面光学性质的变化主要集中在低能区,即低能区的吸收系数和光电导率显著增加.可见,改变厚度和引入缺陷能够有效地调控Si/SiO2界面体系的电子和光学性质,上述研究结果为Si/SiO2界面材料的设计与应用提供了一定的理论依据.  相似文献   

10.
采用基于密度泛函理论的平面波超软赝势方法,在局域密度近似( LDA)下研究了Si纳米层厚度和O空位缺陷对Si/SiO2界面电子结构及光学性质的影响.电子结构计算结果表明:在0.815~2.580nm的Si层厚度范围内, Si/SiO2界面结构的能隙随着厚度减小而逐渐增大,表现出明显的量子尺寸效应,这与实验以及其他理论计算结果一致;三种不同的O空位缺陷的存在均使得Si/SiO2界面能隙中出现了缺陷态,费米能级向高能量方向移动,且带隙有微弱增加.光学性质计算结果表明:随着Si纳米层厚度的减小, Si/SiO2界面吸收系数产生了蓝移; O空位缺陷引入后,界面光学性质的变化主要集中在低能区,即低能区的吸收系数和光电导率显著增加.可见,改变厚度和引入缺陷能够有效地调控Si/SiO2界面体系的电子和光学性质,上述研究结果为Si/SiO2界面材料的设计与应用提供了一定的理论依据.  相似文献   

11.
本文采用第一性原理对纯Al2O3和Si掺杂的Si 0.167Al0.833O1.5, Si 0.25Al0.75O1.5晶体体系的能带结构、态密度进行了计算分析. 结果发现:随着Si在Al2O3晶体中所占比例的增加,体系能隙变小,在Si 0.25Al0.75O1.5晶体体系中能隙已降到2.5eV,表明该体系为半导体材料;而在掺杂的体系中有数条分散的能带穿过了费米能级,即可以预测该掺杂体系有特别的光电性质;同时对比纯Al2O3和Si掺杂的Si 0.167Al0.833O1.5, Si 0.25Al0.75O1.5晶体体系的总态密度,发现掺杂体系的价带和导带向低能区域移动.  相似文献   

12.
本文采用第一性原理对纯Al2O3和Si掺杂的Si0.167Al0.833O1.5,Si0.25Al0.75O1.5晶体体系的能带结构、态密度进行了计算分析.结果发现:随着Si在Al2O3晶体中所占比例的增加,体系能隙变小,在Si0.25Al0.75O1.5晶体体系中能隙已降到2.5 e V,表明该体系为半导体材料;而在掺杂的体系中有数条分散的能带穿过了费米能级,即可以预测该掺杂体系有特别的光电性质;同时对比纯Al2O3和Si掺杂的Si0.167Al0.833O1.5,Si0.25Al0.75O1.5晶体体系的总态密度,发现掺杂体系的价带和导带向低能区域移动.  相似文献   

13.
The electronic structure of silicon carbide with increasing germanium content have been examined using first principles calculations based on density functional theory. The structural stability is analysed between two different phases, namely, cubic zinc blende and hexagonal phases. The zinc blende structure is found to be the stable one for all the Si1-xGexC semiconducting carbides at normal pressure. Effect of substitution of Ge for Si in SiC on electronic and mechanical properties is studied. It is observed that cubic SiC is a semiconductor with the band gap value 1.243?eV. The band gap value of SiC is increased due to the substitution of Ge and the band gap values of Si 0.75 Ge 0.25 C, Si 0.50 Ge 0.50 C, Si 0.25 Ge 0.75 C and GeC are 1.322 eV, 1.413 eV, 1.574 eV and 1.657?eV respectively. As the pressure is increased, it is found that the energy gap gets decreased for Si1-x GexC (X?=?0, 0.25, 0.50, 0.75, 1). The elastic constants satisfy the Born – Huang elastic stability criteria. The bulk modulus, shear modulus, Young’s modulus and Poisson’s ratio are also calculated and compared with the other available results.  相似文献   

14.
The structural and electronic properties of cubic GaN x As1−x with N-concentration varying between 0.0 and 1.0 with step of 0.25 were investigated using the full potential–linearized augmented plane wave (FP-LAPW) method. We have used the local density approximation (LDA) and the generalized gradient approximation (GGA) for the exchange and correlation potential. In addition the Engel-Vosko generalized gradient approximation (EVGGA) was used for the band-structure calculations. The structural properties of the binary and ternary alloys were investigated. The electronic band structure, total and partial density of states as well as the electron charge density were determined for both the binary and their related ternary alloys. The energy gap of the alloys decreases when we move from x=0.0 to 0.25; then it increases by a factor of about 1.8 when we move from 0.25 to 0.5, 0.75 and 1.0 using EVGGA. For both LDA and GGA moving from x=0.0 to 0.25 causes the band gap to close, showing the metallic nature of the GaN0.25As0.75 alloy. When the composition of N moves through x=0.25, 0.5, 0.75 and 1, the band gap increases.  相似文献   

15.
赵龙  芦鹏飞  俞重远  刘玉敏  王东林  叶寒 《中国物理 B》2010,19(5):56104-056104
We perform a first-principles simulation to study the electronic and optical properties of wurtzite Zn1 xCuxO.The simulations are based upon the Perdew-Burke-Ernzerhof form of generalised gradient approximation within the density functional theory.Calculations are carried out in different concentrations.With increasing Cu concentration,the band gap of Zn1 xCuxO decreases due to the shift of valence band.The imaginary part of the dielectric function indicates that the optical transition between O 2p states in the highest valence band and Zn 4s states in the lowest conduction band shifts to the low energy range as the Cu concentration increases.Besides,it is shown that the insertion of Cu atom leads to redshift of the optical absorption edge.Meanwhile,the optical constants of pure ZnO and Zn0.75Cu0.25O,such as loss function,refractive index and reflectivity,are discussed.  相似文献   

16.
基于密度泛函理论(DFT)的第一性原理计算方法,对本征Mn4Si7以及Ge,Al单掺杂和共掺杂Mn4Si7的晶体结构,能带结构,态密度以及光学性质进行了计算和分析.计算结果表明:本征态Mn4Si7的禁带宽度为0.810 eV,为直接带隙半导体材料,掺杂后晶体结构稍微变化,禁带宽度减小,且共掺杂时禁带宽度最小,电导率最好.Al以及Ge,Al共同掺杂时会产生杂质能级.掺杂后光子能量向低能级方向移动,光电导率,光吸收,反射系数都有所增大,说明掺杂改善了Mn4Si7的光学性质,从而可以提高光伏发电效率.  相似文献   

17.
We perform first-principles based on the density function theory to investigate electronic and magnetic properties of 1T-HfS2 monolayer with biaxial tensile strain and compressive strain. The results show that HfS2 monolayer under strains doesn’t display magnetic properties. When the strain is 0%, the HfS2 monolayer presents an indirect band gap semiconductor with the band gap is about 1.252 eV. The band gap of HfS2 monolayer decreases quickly with increasing compressive strain and comes to zero when the compressive strain is above −7%, the HfS2 monolayer system turns from semiconductor to metal. While the band gap increases slowly with increasing tensile strain and comes to 1.814 eV when the tensile strain is 10%. By comparison, we find that the compressive strain is more effective in band engineering of pristine 1T-HfS2 monolayer than the tensile strain. And we notice that the extent of band gap variation is different under tensile strain. The change of band gap with strain from 1% to 5% is faster than that of the strain 6–10%. To speak of, the conduction band minimum (CBM) is all located at M point with different strains. While the valence band maximum (VBM) turns from Γ point to K point when the strain is equal to and more than 6%.  相似文献   

18.
In this paper, electronic and thermoelectric properties of Mg_2C are investigated by using first principle pseudo potential method based on density functional theory and Boltzmann transport equations. We calculate the lattice parameters,bulk modulus, band gap and thermoelectric properties(Seebeck coefficient, electrical conductivity, and thermal conductivity) of this material at different temperatures and compare them with available experimental and other theoretical data. The calculations show that Mg_2C is indirect band semiconductor with a band gap of 0.75 eV. The negative value of Seebeck coefficient shows that the conduction is due to electrons. The electrical conductivity decreases with temperature and Power factor(PF) increases with temperature. The thermoelectric properties of Mg_2C have been calculated in a temperature range of 100 K–1200 K.  相似文献   

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