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1.
The electronic structure and ferromagnetic properties of rutile TiO2 doped with double-impurities Ti1−2xCrxMnxO2 has been investigated using first-principles calculations within the density-functional theory (DFT) and the local density approximation (LDA), functional for treating the effects of exchange and correlation. They were performed using the scalar-relativistic implementation of the augmented spherical wave (ASW). The advantages of doping TiO2 with double impurities instead of single impurities are the increase of the total moment of the system and the exhibition of the half-metallic ferromagnetic nature in Cr- and Mn-doped TiO2 rutile. These behaviors are due to the hybridization of Cr 3d states and nearest-neighboring O 2p states. The spin-spin interaction between magnetic impurities examined by the total energy between parallel and antiparallel aligned states indicated that the Cr and Mn impurities are energetically favorable to be parallel coupled, which mean that the ferromagnetic state is more stable than the ferrimagnetic one. We proposed a bond magnetic polarons (BMP) model, based on localized carriers, to explain the mechanism of ferromagnetism in these systems.  相似文献   

2.
Using the augmented spherical wave method, the electronic structure and magnetic properties of the rutile SnO2 doped with single and double impurities: Sn1−xMnxO2, Sn1−xWxO2, and Sn1−2xMnxWxO2 with x=0.0625, have been studied. The scalar-relativistic implementation with a generalized gradient approximation functional has been used for treating the effects of exchange and correlation. The ground state of Mn-, and W-doped SnO2 systems have a total magnetic moments of 3 and 2 μB, respectively. The half-metallic nature appears in Sn1−2xMnxWxO2, which makes them suitable as spintronic systems with total magnetic moment of 5 μB. The advantages of doping SnO2 with double impurities are investigated in this work. The total moment of the system, the local magnetic moments of the impurities, and their oxidation states are also discussed. Since there are two possible couplings between the impurities, we studied both configurations (ferromagnetic and antiferromagnetic) for double-impurities-doped SnO2. Magnetic properties and interatomic exchange have been computed for various distances between Mn and W. The indirect exchange between double impurities has similarities with the Zener mechanism in transition metal oxides. Based on the interaction between localized moments, via hybridization between impurities orbitals with the host oxygen, a double exchange mechanism is proposed to explain the ferromagnetism of our system.  相似文献   

3.
GeO2 is an enticing candidate to replace SiO2 in electronics industry. To date, no work has appeared in the literature specifically focusing on the (110) facet of rutile GeO2. Density functional theory was applied along with plane-wave approximation to describe the structure and energetics of the (110) plane of tetragonal germanium dioxide. Surface energies were estimated using dispersion-free Perdew–Burke–Ernzerhof (PBE) method as well as dispersion-corrected PBE-D3, D3-corrected revised version of PBE (RPBE-D3), optB88-vdW and optB86b-vdW methods. Atomic displacements with respect to the bulk structure were also reported for slabs relaxed using the aforementioned exchange–correlation functionals. Adsorption energies for weakly bound CO on rutile GeO2(110) surface were also computed using the above-mentioned methods. Vibrational frequency blue-shift of CO as adsorbed onto rutile GeO2(110) surface was also predicted. All the calculated values were comparable to the pertinent literature data, either theoretical or experimental, when available.  相似文献   

4.
N doped TiO is nonmagnetic, in which spin-split impurity states are not induced near the Fermi energy (EF) by N dopant. N doped TiO2 along with transition-metal (TM) doped TiO is magnetic, in which spin-split impurity states are induced across EF. The magnetic moment is determined by the 3d4s electron configurations and the valence states of TM-dopant ions when they substitute Ti. Hence, the origin of ferromagnetism of N doped TiO2 and TiO is not closely related to the width of the band gaps of host oxides, but would be crucially related to that if the dopant can induce spin-split impurity states near EF.  相似文献   

5.
张小超  赵丽军  樊彩梅  梁镇海  韩培德 《物理学报》2012,61(7):77101-077101
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   

6.
杨昌虎  马忠权  徐飞  赵磊  李凤  何波 《物理学报》2010,59(9):6549-6555
采用溶胶-凝胶法在石英玻璃衬底上用旋涂法制备了未掺杂、掺杂钇和掺杂镧的TiO2薄膜样品,对样品在700—1100 ℃范围内进行退火处理,并对样品的拉曼光谱进行了分析.分析表明:随着退火温度的升高,未掺杂TiO2薄膜发生了从锐钛矿相经混相最终向金红石相的转换,掺杂钇和掺杂镧对TiO2薄膜的晶相转换起阻碍作用,掺杂镧的阻碍作用更强;稀土掺杂能使TiO2薄膜晶粒细化,并使晶粒内部应力增大从而阻碍晶格振动,掺杂镧比掺杂钇的效果 关键词: 2薄膜')" href="#">TiO2薄膜 稀土掺杂 拉曼光谱 溶胶-凝胶  相似文献   

7.
8.
The presence of nano-scale lamellae of the α-PbO2-type polymorph of TiO2 sandwiched between twinned rutile inclusions in jadeite has been confirmed by electron diffraction and high-resolution transmission electron microscopy, backed up by image simulation techniques, from ultrahigh-pressure jadeite quartzite at Shuanghe in the Dabie Mountains, China. The crystal structure is orthorhombic with lattice parameters a = 4.58 Å, b = 5.42 Å, c = 5.02 Å and space group Pbcn. A three-dimensional structural model has been constructed for the rutile to α-PbO2-type TiO2 phase transformation based on high-resolution electron microscopic images. Computer image simulation and structural model analysis reveal that rutile {0 1 1}R twin interface is a basic structural unit of α-PbO2-type TiO2. Nucleation of α-PbO2-type TiO2 lamellae 1–2 nm thick is caused by the displacement of one half of the titanium cations within the {0 1 1}R twin slab. This displacement reduces the Ti–O–Ti distance and is favored by high pressure.  相似文献   

9.
Titanium dioxide (TiO2) nanoparticles were modified with poly(methyl methacrylate) (PMMA) to improve the dispersion stability of the nanoparticles in a dielectric medium and to reduce the density mismatch between TiO2 and a dielectric medium for a microcapsule‐type electrophoretic display application. Nanoparticles were coated with PMMA by in situ dispersion polymerization. The PMMA‐coated TiO2 nanoparticles were characterized by fourier transform‐infrared spectrometrey (FT‐IR), electrophoretic light scattering (ELS), and scanning electron microscopy (SEM). Density of PMMA‐coated TiO2 nanoparticles was found to be dependent on the thickness of the PMMA coating on the nanoparticles. An increase of thermal stability of the PMMA layer and the contents of PMMA on the surface of the nanoparticles were measured via thermogravimetric analysis (TGA).  相似文献   

10.
丁万昱  王华林  巨东英  柴卫平 《物理学报》2011,60(2):28105-028105
利用直流脉冲磁控溅射方法在室温下通过改变O2流量制备具有不同晶体结构的N掺杂TiO2薄膜,利用台阶仪、X射线光电子能谱仪、X射线衍射仪、紫外-可见分光光度计等设备对薄膜沉积速率、化学成分、晶体结构、禁带宽度等进行分析.结果表明:所制备的薄膜元素配比约为TiO1.68±0.06N0.11±0.01,N为替位掺杂,所有样品退火前后均未形成Ti—N相结构,N掺杂TiO2薄膜的沉积速率、晶体结构等主要依赖于O2流量.在O2流量为2 sccm时,N掺杂TiO2薄膜沉积速率相对较高,薄膜为非晶态结构,但薄膜内含有锐钛矿(anatase)和金红石(rutile)相晶核,退火后薄膜呈anatase和rutile相混合结构,禁带宽度仅为2.86 eV.随着O2流量的增加,薄膜沉积速率单调下降,退火后样品禁带宽度逐渐增加.当O2流量为12 sccm时,薄膜为anatase相择优生长,退火后呈anatase相结构,禁带宽度为3.2 eV.综合本实验的分析结果,要在室温条件下制备晶态N掺杂TiO2薄膜,需在高O2流量(>10 sccn)条件下制备. 关键词: 2薄膜')" href="#">N掺杂TiO2薄膜 磁控溅射 化学配比 晶体结构  相似文献   

11.
Haowei Peng 《Physics letters. A》2008,372(9):1527-1530
Native point defects in the rutile TiO2 are studied via first-principles pseudopotential calculations. Except for the two antisite defects, all the native point defects have low formation energies. Under the Ti-rich growth condition, high concentrations of titanium interstitials and oxygen vacancies would form spontaneously in p-type samples; whereas high concentrations of titanium vacancies would form spontaneously in n-type samples regardless of the oxygen partial pressure.  相似文献   

12.
采用从头计算二阶自旋-轨道多组态准简并微扰理论计算了碘代甲烷CH3I分子与基态2I03/2和激发态2I0*1/2原子解离极限相关联的势能曲线. 计算了CH3I分子的吸收谱,分析了CH3I分子的光解离过程,并估计了激发态碘原子2I0*3/2的量子产额. 计算结果表明,该方法可用以解释光解离实验结果. 关键词: 3I分子')" href="#">CH3I分子 自旋-轨道耦合 量子产额 光解离  相似文献   

13.
A combined study of IR absorption, photoconductivity, photoluminescence and Raman measurements in ZnO samples supports the theoretical suggestions of a shallow bond-centered hydrogen donor and a shallow hydrogen donor within the oxygen vacancy. In rutile TiO2 we also identify a shallow hydrogen donor in contrast to recent theoretical predictions. A possible solution to this obvious discrepancy is proposed.  相似文献   

14.
This paper describes the synthesis of TiO2 nanoparticles by laser ablation in solution synthesis (Lasis). The laser excimer beam passes through a focusing lens and it is sent to the reaction chamber. The frequency used during the synthesis was 20 Hz, intensity 26 kV The metal ablated by the laser beam undergoes an oxidation process resulting from the reaction with water. We obtain TiO2 nanoparticles with average size of 6.5 nm, crystallized in the rutile structure. The crystallographic and morphological structure was studied by transmission electron microscopy.  相似文献   

15.
王风  王新强  聂招秀  程志梅  刘高斌 《物理学报》2011,60(4):46301-046301
采用基于密度泛函理论(DFT)框架下的第一性原理平面波赝势(PWP)方法,结合广义梯度近似(GGA),对三元化合物ZnVSe2晶体的电子结构进行了计算,分析了ZnVSe2晶体自旋极化的能带结构、电子态密度、电荷布居、磁矩等.计算结果表明,三元化合物ZnVSe2会产生自旋极化状态,能带结构和态密度显示为半金属特征,表现出显著的铁磁性行为,具有高达近100%的传导电子自旋极化率,其半金属能隙为0.443eV,理论预测其可能是一种具有一定应用潜能 关键词: 2')" href="#">ZnVSe2 平面波赝势方法 半金属铁磁性 第一性原理  相似文献   

16.
Ab initio molecular orbital calculations (Hartree–Fock, HF and density functional theories, DFTs) have been carried out for SiO2 polymorphs coesite, low cristobalite, and α-quartz, in order to investigate the reliability of this method for predicting 29Si and 17O nuclear magnetic resonance (NMR) properties of silicates. Oxygen- and silicon-centered clusters consisting of one (1T) to three tetrahedral (3T) shells (one to four atomic shells), taken from real crystal structure, have been investigated. It is found that for reasonable predication of both the 29Si and 17O chemical shifts (δiSi and δiO), the minimum cluster is one that gives the correct second neighbors to the nucleus of interest. Both the δiSi and δiO have reached convergence with respect to cluster size at the OH-terminated two tetrahedral (2T) shell (three atomic shells around Si and four atomic shells around O) model. At convergence, the calculated δiSi values agree well (within ±1 ppm) with experimental data. The calculated 17O electric field gradient (EFG)-related parameters also agree with experimental data within experimental uncertainties. The calculation also reproduces small differences in δiO for O sites with similar tetrahedral connectivities, but shows deviations up to about 10 ppm in relative difference for O sites with different tetrahedral connectivities. The poor performance for the latter is mainly due to the approximations of the HF method. Our study thus suggests that the ab initio calculation method is a reliable mean for predicting 29Si and 17O NMR parameters for silicates. Such an approach should find application not only to well-ordered crystalline phases, but also to disordered materials, by combining with other techniques, such as the molecular dynamics simulation method.  相似文献   

17.
丁芃  刘发民  杨新安  李建奇 《物理学报》2011,60(3):36803-036803
利用直流磁控溅射技术在玻璃衬底上沉积了TiO2薄膜,并对其进行了Co离子注入,最后在真空中500 ℃退火50 min,得到系列薄膜样品. 利用剥离-分散方法制备了薄膜的透射电镜样品,并用扫描电镜(SEM)、X射线能量散射谱(EDX)和高分辨透射电镜(HRTEM)对样品做了近似原位观察,研究了薄膜样品中不同Co离子注入深度的成分分布和显微结构. 结果表明,薄膜呈锐钛矿结构,Co元素主要分布在薄膜表层,Co离子的注入使TiO2薄膜的晶粒被部分破坏,并形成CoO,而5 关键词: 2薄膜')" href="#">Co注入TiO2薄膜 电镜原位观察 室温铁磁性  相似文献   

18.
In this work we have synthesized TiO2 nanoparticles, using either a sol–gel base catalysed process in the interior of CTAB reversed micelles (TiO2 CTAB sol), or the neutralization of a TiO2/H2SO4 solution in the interior of AOT reversed micelles. From the absorption and emission data of the TiO2 nanoparticles it is possible to conclude that in the sol–gel route there remains alkoxide groups in the structure, originating transitions lower than the energy gap of TiO2 semiconductor. These transitions disappear in the neutralization procedure, where the alkoxide groups are absent in the structure. We have assigned the observed indirect and direct optical transitions according to the anatase band structure. TiO2 Langmuir-Blodgett (LB) films were prepared either by direct deposition of titanium isopropoxide or by deposition of the TiO2 CTAB sol. These films showed photoluminescence, which was attributed to band-gap emission and to surface recombination of defect states.  相似文献   

19.
Excess electrons play a key role in many of the properties of Titanium dioxide (TiO2). Understanding their behaviour is important for improving the performance of TiO2 in energy-related applications. Here, we describe a DFT + U study of the locations of the unpaired electron (UPE) on rutile TiO2(110) (R-TiO2(110)) surface and H2O/R-TiO2(110) surface. Our results show that the subsurface are preferred with R-TiO2(110) surface. In contrast to previous studies, we find that the UPE tends to migrate to the surface H2O-Ti5c (the five-coordinated titanium (Ti5c) at surface with H2O adsorption) with the increasing of H2O coverage and UPE concentration. In addition, we have shown that the UPE plays an important role in the O-H bond dissociation and other important elementary reactions in photo-catalytic H2O dissociation on R-TiO2(110) such as H, OH and H2 desorption. Specifically, it enhances the O-H bond dissociation, as well as H and H2 desorption from bridging hydroxyl and Ti5c-OH (the Ti5c with OH adsorption), but hinders the OH and H desorption from Ti5c. We believe our results afford a further understanding of the adsorbent dependent UPE migration, and the role of UPE in the surface reactions.  相似文献   

20.
Electrophoretic deposition (EPD) has been used to combine multi-walled carbon nanotubes of diameter in the range 20–30 nm and commercially available TiO2 nanoparticles (23 nm particle size) in composite films. Laminate coatings with up to four layers were produced by sequential EPD, while composite coatings were obtained by electrophoretic co-deposition of carbon nanotubes and TiO2 nanoparticles, respectively. Scanning electron microscopy was used to characterize the resultant microstructures. The mechanism of EPD of carbon nanotube/TiO2 nanoparticle composites is discussed.  相似文献   

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