SiP化合物结构和电子特性的第一性原理研究

应用第一性原理方法研究了SiP化合物的结构和电子特性,并且将研究推广到其他第四族元素磷化物(IV-P).在研究的各种结构中,SiP单斜晶体结构是能量最低、最稳定的结构.SiP的体弹性模量比CN和CP化合物以及相对应的第三族元素氮化物和磷化物要小.SiP不同的结构间能发生相变,其单斜晶体结构(monoclinic)在压强为6.2 GPa, 15.0 GPa, 19.3 GPa, 20.0 GPa 和 10.3 GPa时分别转变成GeP型结构、Rhom.型结构、β-InS型结构、 CsCl型结构和NaCl型结构.能带计算结果显示SiP单斜晶体结构(monoclinic)和GaSe型结构是间接带隙分别为1.123 eV 和 0.123 eV的半导体,SiP其他结构则显示出金属特性.其他化学比为1:1的第四族元素磷化物(IV-P)具有相同的性质.     

TiO_2纳米管电子结构和光学性质的第一性原理研究

运用基于密度泛函理论的第一性原理方法,系统研究了小尺寸锐钛矿相(n,0)型Ti O2纳米管(D16)的几何构型、电子结构和光学性质.结果表明:随着管径增大,体系单位Ti O2分子的形成能降低,体系趋于稳定;在管径14左右,(n,0)型Ti O2纳米管会发生一次构型的转变.能带分析显示,Ti O2纳米管的电子态比较局域化,小管径下(D14)其导电性更好;随着构型的转变,Ti O2纳米管由直接带隙转变为间接带隙,并且带隙值随着管径的增大而增大,这是由于π轨道重叠效应的影响大于量子限域效应所导致的结果.两种效应的竞争,使得Ti O2纳米管的介电函数虚部ε2(ω)谱的峰值位置随管径增大既可能红移也可能蓝移,管径大于9(即(8,0)管)之后,Ti O2纳米管的光吸收会出现明显的增强.     

掺氮碳化硅纳米管电子结构的第一性原理研究

采用基于密度泛函理论的第一性原理计算,对本征碳化硅纳米管和掺氮碳化硅纳米管的电子结构进行了计算.计算表明本征（8,0）碳化硅为直接带隙半导体,能带间隙为0.94 eV;掺氮浓度为1.56%和3.12％的碳化硅纳米管的能带间隙减小为0.83 eV和0.74 eV.从差分电荷密度可以看出,能带间隙的减小是氮硅键与碳硅键相比共价成键能力降低的结果. 关键词： 碳化硅纳米管 掺氮 第一性原理 电子结构     

β-碳化硅/碳纳米管核壳结构的第一性原理研究

采用基于密度泛函理论的第一性原理方法研究了β-碳化硅/(15, 0) 碳纳米管和β-碳化硅/(16, 0)碳纳米管核壳结构的电子结构特性. 结果表明, 两种核壳异质结构都呈现出金属性, 它们的金属性主要是由碳纳米管和碳化硅纳米线表面的原子所贡献的. 碳化硅纳米线表面呈现的金属性由其结构本身决定, 而对于金属性的 (15, 0) 和半导体性的 (16, 0) 碳纳米管在填充碳化硅纳米线之后都表现出金属性, 主要是由于碳纳米管和碳化硅纳米线之间的电荷转移导致的, 而并不是由于碳纳米管形变造成的. 关键词： 核壳结构 电子结构 第一性原理     

插层化合物Ag1/4TiSe2电子结构的第一性原理研究

采用基于密度泛函理论的平面波赝势方法,选用局域密度近似对Ag1/4TiSe2及TiSe2的几何结构进行了优化和总能量计算.计算得到的晶格常量与实验结果符合较好,负的形成能表明有序Ag1/4TiSe2系统的稳定性.布居数、键长、能带结构和态密度的计算结果显示:Ag以较强的离子性结合于Ag1/4TiSe2中.Ag的插入使得半金属性的TiSe2变为金属性的Ag1/4TiSe2,导电性质得到明显改善.     

铝氮共掺杂氧化锌纳米管电子结构的第一性原理研究

采用基于密度泛函理论的第一性原理计算, 对(6,0)单壁氧化锌纳米管、铝掺杂、氮掺杂和铝氮共掺杂纳米管的能带结构、态密度和差分电荷密度进行了研究. 结果表明, 氮掺杂可以在纳米管禁带中引入受主能级, 实现纳米管的p型掺杂, 但是受主能级局域性较强, 导致氮溶解度低. 引入铝元素可以有效降低氮形成受主能级局域性, 激活氮元素, 铝氮共掺杂有望成为氧化锌纳米管一种更为有效的p型掺杂方法. 关键词： 氧化锌纳米管 电子结构 共掺杂 第一性原理计算     

C/SiC纳米管异质结电子结构的第一性原理研究

采用基于密度泛函理论的第一性原理计算,对扶手椅型(4,4)和(6,6)及锯齿型(8,0)和(10,0)C/SiC纳米管异质结的电子结构进行了研究.结果表明两类异质结结构都表现为半导体特性.扶手椅型纳米管异质结形成了Ⅰ型异质结,电子和空穴都限制在碳纳米管部分.锯齿型纳米管异质结中价带顶主要分布在碳纳米管部分及C/SiC界面处,而导带底均匀分布在整个纳米管异质结上.这两种异质结结构在未来纳米器件中具有潜在的应用价值. 关键词： C/SiC纳米管异质结 第一性原理 电子结构     

FeVO_4电子结构的第一性原理研究

采用基于密度泛函理论的第一性原理方法研究了三斜结构FeVO_4的结构,基态的能带结构、总态密度和分波态密度.将FeVO_4非共线的螺旋磁结构简化为六种不同的反铁磁结构,通过比较不同自旋构型的总能确定了基态磁结构.能带计算和总态密度结果均显示FeVO_4是能隙为2.19 e V的半导体,与实验结果相符.考虑Fe原子的在位库仑能,FeVO_4的能带结构和态密度都发生变化,说明FeVO_4晶体是一个典型的强关联电子体系.     

铁原子吸附联苯烯单层电子结构的第一性原理

联苯烯单层由碳原子的四元、六元和八元环组成,具有与石墨烯相似的单原子层结构.2021年5月,Science首次报道了该材料的实验合成,引起了科研工作者的极大关注.基于第一性原理的密度泛函方法,研究了铁原子在联苯烯单层的吸附构型并分析了其电子结构.结构优化、吸附能和分子动力学的计算表明,联苯烯单层的四元环空位是铁原子最稳定的吸附位点,吸附能可达1.56 eV.电子态密度计算表明铁3d电子与碳的2p电子有较强的轨道杂化,同时电荷转移计算显示铁原子向近邻碳原子转移的电荷约为0.73个电子,说明联苯烯单层与吸附的铁原子之间形成了稳定的化学键.另外,铁原子吸附于联苯烯单层后体系显磁性,铁原子上局域磁矩大小约为1.81μB,方向指向面外.因此,本文确认了联苯烯单层是比石墨烯更好的铁原子吸附载体且体系有磁性,这为研究吸附材料的电磁、输运、催化等特性提供了新的平台.     

Cu台阶面多层弛豫的第一性原理研究

采用基于密度泛函理论的第一性原理赝势平面波方法对Cu(311),(511),(331)和(221)四个高指数台阶表面的弛豫结构和弛豫后表面各层的电子特性进行了系统研究.发现四个台阶面的层间弛豫规律依次为-+-…,--+-…,--+-…和---+-…,与其平台-阶梯n(hkl)×(uvw)的表示法2(100)×(111),3(100)×(111),3(111)×(111)和4(111)×(111)中的原子排数n相关,即     

First-principles study on the structural and electronic properties of ultrathin ZnO nanofilms

Using first-principles density-functional calculations, we have studied the structural and electronic properties of ultrathin ZnO {0001} nanofilms. The structural parameters, the charge densities, band structures and density of states have been investigated. The results show that there are remarkable charge transfers from Zn to O atoms in the ZnO nanofilms. All the ZnO nanofilms exhibit direct wide band gaps compared with bulk counterpart, and the gap decreases with increased thickness of the nanofilms. The decreased band gap is associated with the weaker ionic bonding within layers and the less localization of electrons in thicker films. A staircase-like density of states occurs at the bottom of conduction band, indicating the two-dimensional quantum effects in ZnO nanofilms.     

First-principles study on structural and electronic properties of copper nanowire encapsulated into GaN nanotube

We present a systemic study of the structural and electronic properties of Cu_n nanowires (n=5, 9 and 13) encapsulated in armchair (8,8) gallium nitride nanotubes (GaNNTs) using the first-principles calculations. We find that the formation processes of these systems are all exothermic. The initial shapes are preserved without any visible changes for the Cu₅@(8,8) and Cu₉@(8,8) combined systems, but a quadratic-like cross-section shape is formed for the outer nanotube of the Cu₁₃@(8,8) combined system due to the stronger attraction between nanowire and nanotube. The electrons of Ga and N atoms in outer GaN sheath affect the electron conductance of the encapsulated metallic nanowire in the Cu₁₃@(8,8) combined system. But in the Cu₅@(8,8) and Cu₉@(8,8) combined systems, the conduction electrons are distributed only on the copper atoms, so charge transport will occur only in the inner copper nanowire, which is effectively insulated by the outer GaN nanotube. Considering the maximal metal filling ratio in nanotube, we know that the Cu₉@(8,8) combined system is top-priority in the ultra-large-scale integration (ULSI) circuits and micro-electromechanical systems (MEMS) devices that demand steady transport of electrons.     

高压下LiNbO_3晶体电子结构与光学性质的第一性原理研究

利用基于密度泛函理论的第一性原理超软赝势平面方法研究了外界压强对LiNbO_3晶体态密度,能带结构,电荷密度以及光学性质的影响.能带结构计算表明,价带顶主要由O-2p和Nb-4d态电子贡献,导带底主要由Nb-4d态电子贡献,且带隙随着压强的增加而线性增大.利用复介电函数计算了LiNbO_3晶体在不同压强下光学性质的折射率、反射率、吸收函数,能量损失函数以及光电导率.研究发现:外界压强大于10GPa时,静态折射率保持不变,随外界压强的增加,反射率、吸收函数以及光电导率区间有一定程度的拓宽,损失函数峰发生"蓝移".研究表明,外界高压可以有效调控LiNbO_3晶体的电子结构和光学性质,为LiNbO_3晶体的高压应用提供了有益的理论依据.     

高压下LiNbO3晶体电子结构与光学性质的第一性原理研究

利用基于密度泛函理论的第一性原理超软赝势平面方法研究了外界压强对LiNbO3晶体波态密度,能带结构,电荷密度以及光学性质的影响.能带结构计算表明,价带顶主要由O-2p和Nb-4d态电子贡献,导带底主要由Nb-4d态电子贡献,且带隙随着压强的增加而线性增大.利用复介电函数计算了LiNbO3晶体在不同压强下光学性质的折射率、反射率、吸收系数,能量损失函数以及光电导率. 研究发现：外界压强大于10Gpa时,静态折射率保持不变,随外界压强的增加,反射率、吸收函数以及光电导率区间有一定程度的拓宽,损失函数峰发生“蓝移”.研究表明,高压可以有效调控LiNbO3晶体的电子结构和光学性质,为LiNbO3晶体的高压应用提供了有益的理论依据.     

First-principles study of the electronic and optical properties of ZnO nanowires

The geometric, energetic, electronic structures and optical properties of ZnO nanowires (NWs) with hexagonal cross sections are investigated by using the first-principles calculation of plane wave ultra-soft pseudo-potential technology based on the density functional theory (DFT). The calculated results reveal that the initial Zn-O double layers merge into single layers after structural relaxations, the band gap and binding energies decrease with the increase of the ZnO nanowire size. Those properties show great dimension and size dependence. It is also found that the dielectric functions of ZnO NWs have different peaks with respect to light polarization, and the peaks of ZnO NWs exhibit a significant blueshift in comparison with those of bulk ZnO. Our results gives some reference to the thorough understanding of optical properties of ZnO, and also enables more precise monitoring and controlling during the growth of ZnO materials to be possible.     

镍掺杂硅纳米线电子结构和光学性质的第一性原理研究

利用基于密度泛函理论的第一性原理计算,对镍掺杂硅纳米线的结构稳定性、电子与光学性质进行了研究.结果表明:Ni容易占据硅纳米线表面的替代位置.镍掺杂后的硅纳米线引入了杂质能级,杂质能级主要来源于Ni的3d电子的贡献.由于Ni的3d态和Si的3p态的耦合作用,使禁带宽度变窄.掺杂后的硅纳米线在低能区出现了一个较强的吸收峰,且吸收带出现宽化现象. 关键词： 硅纳米线 掺杂 电子结构 光学性质     

First-principles study on structural and electronic properties of AlNSix heterosheet

Under generalized gradient approximation (GGA), the structural and electronic properties of AlN and Si sheets, hydrogen terminated AlN and Si nanoribbons with hexagonal morphology and 2, 4, 6 zigzag chains across the ribbon width and the hexagonally bonded heterosheets AlNSi_x (x=2, 4, and 6) consisting of hexagonal networks of AlN (h-AlN) strips and silicene sheets with zigzag shaped borders have been investigated using the first-principles projector-augmented wave (PAW) formalism within the density function theory (DFT) framework. The AlN sheet is an indirect semiconductor with a band gap of 2.56 eV, while the Si sheet has a metallic character since the lowest unoccupied conduction band (LUCB) and the highest occupied valence band (HOVB) meet at one k point from Γ to Z. In the semiconductor 6-ZAlNNR, for example, the states of LUCB and HOVB at zone boundary Z are edge states whose charges are localized at edge Al and N atoms, respectively. In metallic 6-ZSiNR, a flat edge state is formed at the Fermi level E_F near the zone boundary Z because its charges are localized at edge Si atoms. The hybridizations between the edge states of h-AlN strips and silicene sheets result in the appearance of border states in the zigzag borders of heterosheets AlNSi_x whose charges are localized at two atoms of the borders with either bonding or antibonding π character.     

Exploration the p-type doping mechanism of GaAs nanowires from first-principles study

Using first-principle calculations, we present a systematic investigation upon the influence of p-type doping on the structural and electronic properties of H-passivated GaAs nanowires with wurtzite structure. The GaAs nanowire models of different doping types, different doping elements, different doping positions and different doping concentrations are established. The calculated formation energies show that Zn element becomes more competitive or even slightly favored in realizing p-type doping compared to Be element. For an individual Zn incorporation model, Zn atom tends to substitute the subsurface Ga atom. As increasing Zn doping concentration, the p-type doping process becomes more and more difficult. Besides, both interstitial and substitutional doping lead to the distortion of atomic structure near impurity atoms and cause the ionicity of GaAs nanowires enhanced. The p-type doped GaAs nanowires models are all direct band gap semiconductors. After substitutional doping, the total density of state curves shift toward higher energy sides and the Fermi level entering valence bands. Our calculations provide a significant reference for the preparation of p-type doping GaAs nanowire, which has a promising potential application in the field of photocathodes.     

Structural and electronic properties of copper nanowire encapsulated into BeO nanotube: First-principles study

We present a systematic study on the structural and electronic properties of close-packed Cu nanowires encapsulated in a series of zigzag (n,0) BeONTs using first-principles calculations. The initial shapes (cylindrical CuNWs and BeONTs) are preserved without any visible changes for the Cu_m@(n,0) (m=6 or 8, 8≤n≤14) combined systems. The most stable combined systems are Cu₆@(10,0) and Cu₈@(11,0) with an optimal tube-wire distance of about 2.8 Å and a simple superposition of the band structures of their components near the Fermi level. A quantum conductance of 3G₀ is obtained for both Cu₆ and Cu₈ nanowires in either free-standing state or filled into BeONTs. The electron transport will occur only through the inner CuNW and the inert outer BeONT serves well as insulating cable sheath. So the Cu₆@(10,0) and Cu₈@(11,0) combined systems is top-priority in the ULSI circuits and MEMS devices that demand steady transport of electrons.