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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,在同等环境条件下,建立了未掺杂和三种不同浓度的Al原子取代Zn原子的Zn1-xAlxO模型,然后分别对模型进行了几何结构优化、总态密度分布和能带分布的计算.结果表明:ZnO高掺杂Al的条件下,随掺杂Al原子浓度增大,进入导带的电子增多,电子迁移率减小,电导率减小,导电性能减弱;但是随高掺杂Al的浓度减小,反而使电子迁移率增大,电导率增大,导电性能增强.计算得到的结果与实验中Al原子
关键词:
Al高掺ZnO
电导率
浓度
第一性原理 相似文献
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采用基于密度泛函理论框架下的第一性原理平面波超软赝势方法,建立了不同Eu掺杂量的锐钛矿相TiO2超胞模型,计算了其态密度、差分电荷密度、能带结构和吸收光谱.结果发现:掺杂后Eu在TiO2的禁带中产生杂质能级.通过对比两种不同Eu掺杂量(1.39at%和2.08at%)下的锐钛矿TiO2的能带结构,发现掺杂量越高,杂质能级越向深能级方向移动,说明电子复合率随杂质浓度增加而增加,即电子寿命变小,同时吸收光谱红移越显著,强度越强.根据实际需要,可在锐钛矿TiO2中适量掺杂Eu,在适当减少电子寿命情况下,使吸收光谱红移. 相似文献
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基于密度泛函理论框架下的第一性原理平面波超软赝势方法, 构建了未掺杂与相同掺杂浓度的Zn1-xTMxO (TM=Al, Ga, In) 超胞模型,分别对模型进行了几何结构优化、态密度分布和能带分布的计算. 结果表明, 分别高掺杂 (Al, Ga, In) 相同原子分数3.125 at%的条件下, In掺杂对ZnO导电性能最好的结果, 计算结果和实验结果相一致.
关键词:
(Al,Ga,In) 高掺ZnO
导电性能
第一性原理 相似文献
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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, 建立了未掺杂与不同浓度的Mn原子取代Zn原子的三种Zn1-xMnxO超胞模型, 分别对模型进行了几何结构优化、态密度分布、能带分布和吸收光谱的计算. 结果表明: 电子非自旋极化处理的条件下, Mn掺杂浓度越小, ZnO形成能越小, 掺杂越容易, 晶体结构越稳定; Mn的掺入使得ZnO体系的杂质能带和导带发生简并化, 并且导带底和价带底同时向低能方向移动, 掺杂后的导带比价带下降得少导致禁带宽度变宽, ZnO吸收光谱明显出现蓝移现象, 计算结果和实验结果相一致. 同时, 电子自旋极化处理的条件下, 体系有磁性, 吸收光谱发生红移现象. 计算结果与相关实验结果相符合. 相似文献
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利用第一原理平面波赝势法, 对(InAs)1/(GaSb)1超晶格原子链的原子结构、力学特性、电子能带结构、 声子结构和光学特性进行研究, 并结合密度泛函理论数值原子轨道赝势法和非平衡格林函数法计算量子输运特性. 与二维层结构的(InAs)1/(GaSb)1超晶格相比, (InAs)1/(GaSb)1超晶格原子链的能带结构有明显不同, 在某些情况下表现为金属能带特性. 对理想条件下(InAs)1/(GaSb)1 超晶格原子链的力学强度计算表明, 该结构可承受的应变高达 ε=0.19. 通过对声子结构的完整布里渊区分析, 研究了(InAs)1/(GaSb)1超晶格原子链的结构稳定性. 对两端接触电极为Al纳米线的InAs/GaSb超晶格原子链的电子输运特性计算表明, 电导随链长和应变的改变而发生非单调变化.光吸收谱的计算结果表现出在红外波段具有陡峭吸收边, 截止波长随超晶格原子链的结构而变化.预计InAs/GaSb超晶格原子链可应用于红外光电子纳米器件, 通过改变超晶格原子链的结构来调节光电响应波段. 相似文献
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采用密度泛函理论平面波超软赝势方法, 计算并分析了Mo/X(B, C, N, O, F)共掺杂TiO2体系的形成能、电子结构和光学性质, 研究了共掺杂协同效应对于计算体系光催化性能的影响机制. 首先计算出不同掺杂体系的态密度及能带结构, 利用能带理论分析了共掺杂效应对于禁带宽度的调控作用, 进而分析了共掺杂对TiO2光催化能力和稳定性的协同作用. 结合电荷密度图, 分析原子间的电荷转移情况, 得到计算体系中各原子成键状态. 最后, 结合光吸收谱线分析得出Mo/C共掺杂类型在调制TiO2体系中可见光波段的光催化性能上优势明显, 在催化作用上表现出协同效应. 本文的理论研究对共掺杂方法在TiO2光催化领域有着一定的指导意义. 相似文献
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采用基于密度泛函理论的平面波赝势方法和广义梯度近似,对未掺杂、掺B、掺N的碳纳米管(CNT)不同位置上Al原子的吸附进行了几何优化,计算了吸附Al、掺杂前后CNT的能带结构、态密度、差分电荷密度、电荷布居数和吸附能.计算结果表明,掺B使CNT形成缺电子状态,利于具有自由电子的Al原子的吸附结合,可显著提高Al在金属性的(5,5)CNT和半导性的(8,0)CNT外壁的吸附能;掺杂N形成多电子状态,在费米能级附近半满的施主能级也利于填充Al的价电子,改善Al在(5,5)CNT和(8,0)CNT外壁的吸附结合性
关键词:
密度泛函理论
单壁碳纳米管
B(N)掺杂
Al原子吸附 相似文献
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《Current Applied Physics》2015,15(11):1556-1561
In this paper, first-principles calculations have been implemented to study the structural relaxation, formation energies and electronic structure of Al doped α-MnO2. Both Al insertion and Al substitution reactions in the α-MnO2 were considered. Calculated formation energies indicate that Mn atom is easier to be displaced by Al atom under the O-rich growth condition compared with Al insertion reaction. Besides, it can be found that Al doping can afford acceptor impurity level which can accommodate electrons, thus contributing to the improvement of conductivity of α-MnO2. The conductivity of α-MnO2 is gradually improved with the increasing doping concentration of Al, and Al0.0417Mn0.9583O2 exhibits the best conductivity. Lastly, the electronic structure of Al0.0417Mn0.9583O2 was further investigated by analysis of total charge density and Bader charge. It is clear that Al doping can afford more electrons for α-MnO2, which also contributes to improvement of its conductivity. 相似文献
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采用基于密度泛函理论的平面波赝势方法对SnO2:F体系的电子结构进行了第一性原理模拟计算.用广义梯度近似方法优化SnO2:F体系的晶胞结构,计算了体系基态总能.通过确定F掺杂对O的优先替代位置,计算了SnO2:F的能带结构、态密度、分波态密度.分析了F掺杂对SnO2晶体的电子结构和晶体性质及光学吸收边的影响,从理论上得出光学吸收边发生蓝移.对不同掺杂量的体系电子结构进行了分析.
关键词:
F掺杂
2')" href="#">SnO2
电子结构
态密度 相似文献
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本文采用基于密度泛函理论(DFT)的第一性原理计算了铂原子填充扶手椅型石墨烯纳米带(AGNR)中双空位结构的电学性能.计算结果表明: 通过控制铂原子的掺杂位置, 可以实现纳米带循环经历小带隙半导体—金属—大带隙半导体的相变过程; 纳米带边缘位置是铂原子掺杂的最稳定位置, 边缘掺杂纳米带的带隙值随宽度的变化与本征AGNR一样可用三簇曲线表示, 但在较大宽度时简并成两条曲线, 一定程度上抑制了带隙值的振荡; 并且铂原子边缘掺杂导致宽度系数Na = 3p和3p + 1(p是一个整数)的几个较窄纳米带的带隙中出现杂质能级, 有效地降低了其过大的带隙值. 此外, 铂掺杂AGNR的能带结构对掺杂浓度不是很敏感, 从而降低了对实验精度的挑战. 本文的计算有利于推动石墨烯纳米带在纳米电子学方面的应用. 相似文献
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First-principle study on the effect of high Li-2N co-doping on the conductivity of ZnO 总被引:1,自引:0,他引:1
Based on the density functional theory (DFT), using first-principles plane-wave ultrasoft pseudopotential method, the models of the unit cell of pure ZnO and two highly Li-2N co-doped supercells of Zn0.9375Li0.0625O0.875N0.125 and Zn0.9167Li0.0833O0.8333N0.1667 were constructed, and the geometry optimization for the three models was carried out. The total density of states (TDOS) and the band structures (BS) were also calculated. The calculation results showed that in the range of high doping concentration, when the co-doping concentration is more than a certain value, the conductivity decreased with the increase of co-doping concentration of Li-2N in ZnO, which agrees with the change trend of the experimental results. 相似文献
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采用基于密度泛函理论(DFT)框架下的第一性原理平面波超软赝势方法,在同等环境条件下,建立了不同大小的ZnO模型,在ZnO中对不同浓度的氮和铝原子进行了高掺杂,并对低温条件下高掺杂氮和铝原子的ZnO半导体进行了态密度计算,然后分别对进入价带的相对空穴数和空穴散射迁移率进行了计算,最后对电导率进行了类比,发现适量低浓度的高掺杂氮和铝原子会使ZnO半导体的导电性能增强.即在低温高掺杂氮和铝原子的条件下,ZnO半导体的电导率不仅与掺杂氮和铝原子浓度有关,而且和进入价带的相对空穴数有关.和空穴散射的迁移率有关的结
关键词:
ZnO半导体
浓度
电导率
第一性原理 相似文献
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To deeply understand the effects of Si/N-codoping on the electronic structures of TiO2 and confirm their photocatalytic performance, a comparison theoretical study of their energetic and electronic properties was carried out involving single N-doping, single Si-doping and three models of Si/N-codoping based on first-principles. As for N-doped TiO2, an isolated N 2p state locates above the top of valence band and mixes with O 2p states, resulting in band gap narrowing. However, the unoccupied N 2p state acts as electrons traps to promote the electron-hole recombination. Using Si-doping, the band gap has a decrease of 0.24 eV and the valence band broadens about 0.30 eV. These two factors cause a better performance of photocatalyst. The special Si/N-codoped TiO2 model with one O atom replaced by a N atom and its adjacent Ti atom replaced by a Si atom, has the smallest defect formation energy in three codoping models, suggesting the model is the most energetic favorable. The calculated energy results also indicate that the Si incorporation increases the N concentration in Si/N-codoped TiO2. This model obtains the most narrowed band gap of 1.63 eV in comparison with the other two models. The dopant states hybridize with O 2p states, leading to the valence band broadening and then improving the mobility of photo-generated hole; the N 2p states are occupied simultaneously. The significantly narrowed band gap and the absence of recombination center can give a reasonable explanation for the high photocatalytic activity under visible light. 相似文献
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First-principles calculations for intrinsic and Zn-doped In0.25Ga0.75As are performed based on density functional theory to study the influence of Zn doping on electronic and optical properties. The band structure, density of state, Mulliken population, dielectric function, complex refractive index, absorption coefficient and reflectivity of In0.25Ga0.75As are calculated. Results show that the Fermi levels of two Zn-doped models enter into the valence bands and Zn atom is more easily to replace In atom than Ga atom. The lattice constant of In0.2344Ga0.75Zn0.0156As reduced after optimization, while that of In0.25Ga0.7344Zn0.0156As increased to the contrary. The Mulliken bond population shows that the doping Zn atoms can enlarge the strength of In–As and Ga–As polar covalent bonds. Furthermore, the calculated absorption coefficient and reflectivity are used to characterize the performance of photoemission, indicates that the photoresponses of Zn-doped models are better than that of the intrinsic. 相似文献