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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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运用第一性原理,对C掺杂锐钛矿相TiO2的电子结构进行了研究,从能带结构理论解释了C掺杂TiO2吸收光谱的一些实验现象.发现在C掺杂后的锐钛矿相TiO2的禁带宽度增大,并且在带隙中出现了杂质能级,这些杂质能级主要是由C 2p轨道上的电子构成的,它们之间是独立的,正是这些独立的杂质能级使TiO2掺杂后可以发生可见光响应.价带上的电子可以吸收一定能量的光子跃迁到杂质能级,而杂质能级上的电子也可以吸收一定能量的光子跃迁到导带,所以从理论上可以计算出掺杂后的TiO2在可见光范围内存在两个吸收边,与实验中所得到的现象相一致. 相似文献
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近年来的理论和实验研究表明,通过不同离子共掺杂TiO2是减小其禁带宽度的一种有效方法.本文采用基于第一性原理的平面波超软赝势方法研究了C和Zn共掺杂TiO2的能带结构、态密度和光学性质.计算结果表明C-Zn共掺杂导致导带相对Fermi能级发生了明显的下降,同时在TiO2的导带下方与价带上方形成了新的杂质能级,使TiO2的禁带宽度变小, TiO2的光学吸收带边产生红移. 杂质能级可以降低光激发产生的电子-空穴对的复合概率, 提高TiO2的光催化效率. 此外, 掺杂后TiO2在可见光区的吸收系数有明显增加, 能量损失也明显减小. 相似文献
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采用基于密度泛函理论的第一性原理方法对未掺杂以及不同浓度过渡金属Fe,Co,Ni,Zn掺杂金红石TiO2的超晶胞体系进行了几何优化,并讨论了其晶格常数,电子能带结构和光学性质.研究结果表明:掺杂前后的晶格参数与实验值偏差在3.6%以下;适量的过渡金属掺杂不但影响体系能带结构,拓宽光吸收范围,而且扮演着俘获电子的重要角色,有利于光生电子-空穴对的有效分离以及增强光吸收能力;Fe,Co,Ni,Zn最佳理论掺杂体系分别为Ti0.75Fe0.25O2,Ti0.75Co0.25O2,Ti0.75Ni0.25O2,Ti0.83Zn0.17O2;Fe,Co,Ni3d态分裂为t2g和eg态,分别贡献于价带高能级和导带低能级部分,促进了电子-空穴对的生成,从而可提高TiO2的光催化性能;Zn3d态电子成对填满轨道,不易被激发,故光催化活性无明显提高. 相似文献
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采用基于密度泛函理论的平面波超软赝势方法研究了纯锐钛矿相TiO2及掺杂3d过渡金属TiO2的几何、电子结构及光学性质. 计算结果表明掺杂能级的形成主要是掺杂过渡金属3d轨道的贡献,掺杂能级在禁带中的位置是决定TiO2吸收带边能否出现红移的重要因素. Cr,Mn,Fe,Ni,Co,Cu掺杂使TiO2的吸收带边产生红移,并在可见光区有一定的吸收系数; Sc,Zn掺杂使TiO2的吸收带边产生蓝移,但在可见光区有较大的吸收系数;掺V不但使TiO2的吸收带边产生红移,增强了在紫外光区的光吸收,而且在可见光区有非常大的吸收系数. 相似文献
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提出了一种利用离子注入和后续退火制备氮掺杂TiO2薄膜的方法。首先在室温下向石英玻璃中注入Ti离子,随后在氮气中退火到900 ℃,从而制备了氮掺杂的玻璃基TiO2薄膜。SRIM2006程序模拟和卢瑟福背散射谱(RBS)研究表明注入离子从样品表面开始呈高斯分布,实验结果和模拟结果吻合很好。X射线光电子能谱(XPS)研究结果表明注入态样品中形成了金属Ti和TiO2,900 ℃退火后金属Ti转变成TiO2,同时N原子替代少量的晶格O原子形成了O-Ti-N化合物。紫外-可见吸收光谱(UV-Vis)结果显示,当退火温度至500 ℃时,在吸收光谱中开始出现TiO2的吸收边,随退火温度升高到900 ℃,由于O-Ti-N化合物形成,TiO2的吸收边从3.98 eV红移到3.30 eV,TiO2吸收边末端延伸到可见光区,在可见光区的吸收强度明显增加。 相似文献
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采用第一性原理平面波超软赝势方法研究了N,Co共掺杂锐钛矿相TiO2的微观结构和光学性质.结果表明:N,Co共掺杂后TiO2晶格中产生的偶极矩使光生电子-空穴对更有效地分离;在TiO2导带和价带之间形成了新的杂质能级,一方面使吸收带边红移到可见光区,光吸收性能明显增强,另一方面有利于光生电子-空穴对的分离,提高TiO2的光量子效率;与纯TiO2相比,N,Co共掺杂锐钛矿相TiO2带边的氧化还原势只有微小的变化,共掺杂后TiO2的强氧化还原能力得以保持. 相似文献
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采用第一性原理平面波超软赝势方法,系统研究了Mn,N共掺杂对锐钛矿相TiO2的晶体结构、缺陷形成能、电子结构、光学性质以及氧化还原能力的影响.研究表明:Mn,N共掺杂锐钛矿相TiO2后,TiO2晶格发生了畸变,导致晶体八面体偶极矩增加,有利于光生电子-空穴对的有效分离;在TiO2带隙中出现了杂质能级,使锐钛矿相TiO2的光学吸收带边红移,可见光区的吸收系数明显增大,有利于光催化效率的提高;在不考虑
关键词:
2')" href="#">锐钛矿相TiO2
第一性原理
Mn和N共掺杂
光催化性能 相似文献
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The undoped, Fe-doped, N-doped and Fe+N codoped titanium dioxide (TiO2) samples were synthesized. Detailed analysis shows that all the samples are pure anatase with the shape of a nanorod, and N and Fe ions are incorporated into the TiO2 lattice. For all the samples, the saturation magnetization at room temperature is in the order of the Fe+N codoped TiO2>N-doped TiO2>Fe-doped TiO2>undoped TiO2. Upon N doping, enhanced ferromagnetic properties were observed. The N content in Fe+N codoped TiO2 is about two times as large as that in the N-doped TiO2, which may account for the largest saturation magnetization observed in Fe+N codoped TiO2. It is suggested that metal ion and N codoping may provide a new approach for increasing the saturation magnetization in TiO2-based dilute magnetic semiconductors. 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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We present GGA+U calculations to investigate the electronic structure and visible‐light absorption of N,B‐codoped anatase TiO2. The NsBi (substitutional N, interstitial B) codoped TiO2 produces significant Ti 3d and N 2p mid‐gap states when the distance of N and B atoms is far, whereas the NiBi (interstitial N and B) and NsBs (substitutional N and B) codoped TiO2 prefer to form localized p states at 0.3–1.2 eV above the valence band maximum. Further, the optical band edges of the three codoped systems shift slightly to the visible region, but only the far‐distance NsBi codoped TiO2 clearly shows an optical transition. These results indicate that NsBi codoped TiO2 has a dominant contribution to the optical absorption of N,B‐codoped TiO2. (© 2012 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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A strategy of enhancing the photoactivity of TiO2 containing nonmetal and transition metal dopants 下载免费PDF全文
An effective structural codoping approach is proposed to modify the photoelectrochemical (PEC) properties of anatase TiO2 by being doped with nonmetal (N or/and C) and transition metal (Re) elements. The electronic structures and for- mation energies of different doped systems are investigated using spin-polarized density functional theory. We find that (C, Re) doped TiO2, with a low formation energy and a large binding energy, reduces the band gap to a large extent, thus it could contribute to the significant enhancement of the photocatalytic activity in the visible-light region. It should be pointed out that, to be successful, the proper proportion of the dopants C and Re should be controlled, so that reasonable PEC properties can be achieved. 相似文献