氮掺杂石墨烯纳米结构的等离激元激发（英文）

基于含时密度泛函理论,研究了氮掺杂石墨烯纳米结构的等离激元特性。吡啶型氮掺杂不影响石墨烯纳米结构的等离激元激发特性,而取代型氮掺杂主要基于石墨烯纳米结构对称性的改变和体系中电子密度的增加来影响石墨烯纳米结构的等离激元共振。相对于纯六角石墨烯纳米结构,在低能共振区,取代型氮掺杂六角石墨烯纳米结构的等离激元共振能量发生了红移。相对于纯矩形石墨烯纳米结构,在低能共振区,取代型氮掺杂矩形石墨烯纳米结构沿扶手椅型边界方向激发时,其等离激元共振能量发生了蓝移;沿Z字型边界激发时,其主要的等离激元共振模式受掺杂氮的影响较小。     

剪切形变对硼氮掺杂碳纳米管超晶格电子结构和光学性能的影响

碳纳米管作为最先进的纳米材料之一, 在电子和光学器件领域有潜在的应用前景, 因此引起了广泛关注. 掺杂、变形及形成超晶格为调制纳米管电子、光学性质提供了有效途径. 为了理解相关机理, 利用第一性原理方法研究了不同剪切形变下扶手椅型硼氮交替环状掺杂碳纳米管超晶格的空间结构、电子结构和光学性质. 研究发现, 剪切形变会改变碳纳米管的几何结构, 当剪切形变大于12%后, 其几何结构有较大畸变. 结合能计算表明, 剪切形变改变了掺杂碳纳米管超晶格的稳定性, 剪切形变越大, 稳定性越低. 电荷布居分析表明, 硼氮掺杂碳纳米管超晶格中离子键和共价键共存. 能带和态密度分析发现硼氮交替环状掺杂使碳纳米管超晶格从金属转变为半导体. 随着剪切形变加剧, 纳米管超晶格能隙逐渐减小, 当剪切形变大于12%后, 碳纳米管又从半导体变为金属. 在光学性能中, 剪切形变的硼氮掺杂碳纳米管超晶格的光吸收系数及反射率峰值较未受剪切形变的均减小, 且均出现了红移.     

Cr掺杂锐钛矿型TiO_2(001)薄膜中Cr原子的直接观测（英文）

掺杂元素的成像对于理解TiO_2掺杂薄膜的光催化活性是至关重要的.然而,如何在原子尺度上表征掺杂原子与TiO_2晶格之间的相互关联性仍然是一项挑战性工作.本文利用高角环形暗场像/环形明场像扫描透射电镜(HA ADF/ABF-STEM)结合电子能量损失谱(EELS)从[100]晶向上对锐钛矿型Ti02(001)薄膜中掺杂的单个铬原子进行了直接成像.结果表明,Cr掺杂原子同时占据TiO_2晶格中的取代位和填隙位,而其可以用具有原子级分辨的电子能量损失谱元素面分布图(EELS mapping)来成像识别,但在HAADF/ABFSTEM图像中未能被看到.大部分的Cr掺杂原子更倾向于取代TiO_2晶格中的Ti原子.这些结果在原子尺度上为Cr掺杂TiO_2薄膜的掺杂构型提供了直接的证据,同时也表明电子能量损失谱元素面分布图在对掺杂材料的结构表征是个非常出色的技术.     

硼(氮、氟)掺杂对TiO2纳米颗粒光学性能的影响

利用X射线衍射谱、拉曼光谱和紫外-可见光吸收光谱研究了硼(氮、氟)掺杂对TiO₂纳米颗粒光学性能的影响.X射线衍射谱和拉曼光谱结果表明,掺硼(氮、氟)对TiO₂纳米颗粒的锐钛矿相晶体结构无明显影响,而其锐钛矿晶格出现畸变(c/a值增大),这被归因于掺杂原子对TiO₂纳米颗粒表面氧原子缺位沿晶格c轴方向的占据.另外,掺硼(氮、氟)TiO₂纳米颗粒吸收带红移与TiO相似文献   

Be，C双受主共掺杂实现P型AlN的第一性原理研究

基于密度泛函理论 Density Functional Theory 的第一性原理平面波超软赝势方法USPP,首先对Be、C掺杂AlN的晶格结构进行优化,得到其稳定结构．然后对Be、C掺杂AlN的晶格参数、结合能、能带结构、电子态密度和电荷集居数进行了详细地计算和分析．计算结果表明：Be-2C共掺杂AlN的构型具有更稳定的结构,能使受主能级变宽、非局域化特征明显．因此,Be-2C共掺杂AlN有望成为一种更稳定高效的p型掺杂手段．     

S、Cr共掺杂TiO2纳米材料的固相合成及其可见光降解性能

采用固相反应法分别合成了铬掺杂二氧化钛(Cr-TiO2)及硫和铬共掺杂二氧化钛(S-Cr-TiO2)纳米材料.并用XRD、SEM、UV-Vis、XPS、N2吸附等技术对材料进行了物相结构表征,同时研究了材料对水溶苯胺蓝的可见光降解性能.结果表明,在S-Cr-TiO2纳米材料中,硫以阳离子S6+进入二氧化钛晶格或晶格间隙...     

Zn,Ni,Mg高掺杂La1.85Sr0.15CuO4的晶体结构比较

对Zn ,Ni,Mg高掺杂的La1.85Sr0 .15CuO4 (LSCO)超导体的X射线衍射谱进行了仔细的分析 ,从而获得了各掺杂样品的晶格常量、原子结构参量及衍射的峰形参量 ,比较了不同掺杂所引起的晶体结构的差异 ,计算了由于掺杂所产生的晶格内部的微应变 ,结果表明非磁性金属Zn ,Mg掺杂比磁性金属Ni掺杂更强烈地抑制了LSCO的超导电性可能与材料中晶格的微应变有关     

氮掺杂手性碳纳米管的电子结构和输运特性的理论研究

运用第一性原理的密度泛函理论,结合非平衡格林函数,研究了氮原子取代掺杂手性单壁(6,3)碳纳米管的电子结构和输运特性.计算结果表明:不同构形和不同数目的氮原子取代掺杂对手性碳管的输运性质有很复杂的影响.研究发现,氮原子掺杂明显改变了碳管的电子结构,使金属型手性碳管的输运性能降低,电流-电压曲线呈非线性变化,而且输运性能随着杂质原子间间距的变化而发生显著改变.在一定条件下,金属型碳管向半导体型转变. 关键词： 手性单壁碳纳米管 氮掺杂 电子结构 输运性能     

不同氮掺杂浓度碳纳米管的制备及其成键特性分析

采用化学气相沉积法,以吡啶为氮源,乙炔为碳源,制备出了不同氮掺杂含量的碳纳米管.使用透射电子显微镜(TEM)和X射线荧光光谱(XPS)对样品的形貌和成键特性进行了观察和分析.TEM测试发现随着掺杂量的增大,氮掺杂碳纳米管的竹节长度从120 nm减小为40 nm左右,同时管身变得更加弯曲,管壁变得粗糙.XPS测试发现氮元素在碳纳米管中以“吡啶”、“吡咯”和“石墨”三种C—N键合方式存在.结合三种价键的形成原因,分析了氮掺杂浓度对键合形式的影响,并根据价键的存在形式解释了碳纳米管形貌变化的原因. 关键词： 碳纳米管 氮掺杂 XPS     

Co,N共掺杂锐钛矿相TiO2电子结构和光学性质的第一性原理研究

二氧化钛(TiO2)作为一种性能优良的光催化剂已经被广泛地研究和使用. 本研究中利用了第一性原理和GGA+U方法, 对锐钛矿结构TiO2晶体三种可能的(Co,N)共掺杂体系的几何结构、形成能、电子结构和光吸收系数进行了研究, 并与单掺杂(Co/N)体系进行了对比. 结果表明, 在三种共掺杂TiO2中, Co与N相邻时晶格畸变最小, 但掺杂原子周围晶格畸变较大;同时, 较低的形成能表明此种共掺杂结构最容易形成;此外, 因为Co与N成键, 其杂质能级的数目与能量较其他共掺杂结构有较大差异. (Co,N)共掺杂体系与未掺杂TiO2的相比, 其禁带宽度较小, 禁带中存在杂质能级, 因此其吸收边红移, 在可见光波段有较好的光吸收能力. 故(Co,N)共掺杂可以很好地提升锐钛矿型TiO2在可见光波段的光催化性能.     

Preparation of visible light responsive N doped TiO2 via a reduction-nitridation procedure by nonthermal plasma treatment

A visible light responsive N-doped TiO₂ was prepared via a reduction-nitridation procedure by nonthermal plasma treatment. X-ray diffraction, N₂ adsorption, UV-vis spectroscopy, photoluminescence, and X-ray photoelectron spectroscopy were used to characterize the prepared TiO₂ samples. The plasma treatment did not change the phase composition and particle sizes of TiO₂ samples, but extended its absorption edges to the visible light region. The photocatalytic activities were tested in the degradation of an aqueous solution of a reactive dyestuff, methylene blue, under visible light. The photocatalytic activities of TiO₂ prepared by reduction-nitridation procedure were much higher than that of samples prepared by simple nitridation treatment. The enhanced activity was ascribed to the substitutional N-doping and appropriate concentration of oxygen vacancies. TOHN10 prepared by reduction-nitridation procedure exhibited excellent photocatalytic stability. A possible mechanism for the photocatalysis was proposed.     

Effect of N2 ion flux on the photocatalysis of nitrogen-doped titanium oxide films by electron-beam evaporation

Nitrogen-doped titanium oxide (TiO_xN_y) films were prepared with ion-assisted electron-beam evaporation. The nitrogen (N) incorporated in the film is influenced by the N₂ flux modulated by the N₂ flow rate through an ion gun. The TiO_xN_y films have the absorption edge of TiO₂ red-shifted to 500 nm and exhibit visible light-induced photocatalytic properties in the surface hydrophilicity and the degradation of methylene blue. The structures and states of nitrogen in the films are investigated by X-ray diffraction patterns (XRD), and X-ray photoelectron spectroscopy (XPS) and related to their visible light-induced photocatalytic properties. The results indicate that the substitutional N in anatase TiO₂ can induce visible light photocatalysis. The substitutional N is readily doped by the energetic nitrogen ions from the ion gun. The best photocatalytic activity is obtained at the largest N loading about 5.6 at.%, corresponding to the most substitutional N in anatase TiO₂. The film exhibits the degradation of methylene blue with a rate-constant (k) about 0.065 h⁻¹ and retaining 7° water contact angle on the surface under visible light illumination.     

Efficient visible light-induced degradation of phenol on N-doped anatase TiO2 with large surface area and high crystallinity

The N-doped anatase TiO₂ photocatalysts were prepared via solvothermal and ethylenediamine reflux treatment, followed by the sequential calcination in air and NH₃/N₂ atmosphere. The resulting photocatalysts were characterized by X-ray diffraction, X-ray photoelectron spectroscopy, Fourier transform infrared spectroscopy and UV-vis diffuse reflectance spectra. The results revealed that the prepared N-doped anatase TiO₂ had characteristics of small crystallite size, large surface area, high crystallinity and visible light response. The prepared N-doped anatase TiO₂ photocatalysts showed much higher photocatalytic activity than N-doped Degussa P25 for the degradation of phenol under both ultraviolet and visible light irradiation, owing to more highly oxidizing hydroxyl radical which was the main oxidative species responsible for the degradation of phenol.     

An efficient composite growing N-doped TiO<Subscript>2</Subscript> on multi-walled carbon nanotubes through sol–gel process

High-activity, visible-light-driven photocatalysts were prepared by forming N-doped TiO₂ on multi-walled carbon nanotubes (MWCNTs). The use of MWCNTs as the support in a N-doped TiO₂ system favored electron trapping, because the recombination process could be retarded, thus promoting photocatalytic activity. The prepared photocatalysts were systematically characterized by transmission electron microscopy (TEM), X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), Brunaure–Emmett–Teller (BET) spectroscopy, and UV–Vis diffuse reflectance spectroscopy (UV–Vis/DRS). The results indicated that the N-doped TiO₂ coated on MWCNTs improved the surface area and slightly modified the optical properties of the composite. The activities of the photocatalysts were probed by photodegradation of methanol in the presence of visible light irradiation. The experimental results revealed that the strong interphase linkage between the MWCNTs and the N-doped TiO₂ played a significant role in improving photocatalytic activity. However, the mechanical process for MWCNT–TiO_2-x N _x mixtures showed lower activity than just pure N-doped TiO₂. In this study, N-doped TiO₂ precursors coated with pretreated MWCNTs during a sol–gel process could effectively form a MWCNT–TiO_2-x N _x composite. The composite showed excellent activity and effectively enhanced the efficiency of N-doped TiO₂ under the visible light region.     

Synthesis and characteristics of natural zeolite supported Fe-TiO2 photocatalysts

Natural zeolite supported Fe³⁺-TiO₂ photocatalysts were synthesized for the sake of improving the recovery and photocatalytic efficiency of TiO₂. The as-prepared materials were characterized by X-ray diffraction (XRD), fourier transform infrared spectroscopy (FT-IR), X-ray photoelectron spectroscopy (XPS), ultraviolet-visible diffuse reflection spectroscopy (UV-vis DRS), scanning electron microscopy (SEM) and energy-dispersive X-ray analysis (EDX). Methyl orange was used to estimate the photocatalytic activity of the samples. The results showed that zeolite inhibited the growth of TiO₂ crystallite sizes. The Fe³⁺ concentration played an important role on the microstructure and photocatalytic activity of the samples. The iron ions could diffuse into TiO₂ lattice to the form Fe-O-Ti bond and gave TiO₂ the capacity to absorb light at lower energy levels. The photocatalytic activity of the samples could be enhanced as appropriate dosages of Fe³⁺ were doped.     

Preparation and photocatalytic activity of nitrogen-doped TiO2 hollow nanospheres

TiO₂ hollow nanospheres were prepared using silicon oxide as a template. N-doped titanium oxide hollow spheres, TiO_2−xN_x were synthesized by reacting TiO₂ hollow spheres with thiourea at 500 °C. XRD and XPS data showed that oxygen was successfully substituted by nitrogen through the nitrogen-doping reaction, and finally N-doped TiO₂ hollow spheres were formed. The N-doped TiO₂ hollow spheres showed new absorption shoulder in visible light region so that they were expected to exhibit photocatalytic activity in the visible light. The photocatalytic activity of N-doped TiO₂ hollow spheres under visible light was similar to that of normal spherical TiO_2−xN_x in spite of the structural difference.     

P掺杂锐钛矿相TiO2的第一性原理计算

利用基于密度泛函理论的第一性原理对不同P掺杂形式(P替位Ti, P替位O, 间隙P)的锐钛矿相TiO₂的晶格常数、电荷布居、能带结构、分态密度和吸收光谱进行了计算. 结果表明, P替位Ti时, TiO₂体积减小, P替位O和间隙P的存在使TiO₂的体积膨胀; 替位Ti的P和间隙P均有不同程度的氧化, 而替位O的P带有负电荷. 三种P掺杂形式均导致锐钛矿相TiO₂禁带宽度的增大, 并在TiO₂禁带之内引入了掺杂局域能级. P掺杂导致TiO₂禁带宽度增大的程度依次为: 间隙P>P替位Ti>P替位O. 吸收光谱的计算结果表明, P替位Ti并不能增强TiO₂的可见光吸收能力, 但间隙P的存在大幅提高了TiO₂的可见光光吸收能力, 间隙P有可能是造成实验上P掺杂增强锐钛矿相TiO₂光催化活性的重要原因. 关键词： P掺杂 2')" href="#">锐钛矿相TiO₂ 第一性原理     

Preparation of N-doped TiO<Subscript>2</Subscript> photocatalyst by atmospheric pressure plasma process for VOCs decomposition under UV and visible light sources

The nitrogen doped (N-doped) titanium dioxide (TiO₂) photocatalyst was prepared by the atmospheric-pressure plasma-enhanced nanoparticles synthesis (APPENS) process operated under normal temperature, i.e. the dielectric barrier discharge plasma process. The N₂ carrier gas is dissociated in the AC powered nonthermal plasma environment and subsequently doped into the TiO₂ photocatalyst that was capable of being induced by visible light sources. The APPENS process for producing N-doped TiO₂ showed a higher film deposition rate in the range of 60–94 nm/min while consuming less power (<100 W) as compared to other plasma processes reported in literatures. And the photocatalytic activity of the N-doped TiO₂ photocatalyst was higher than the commercial ST01 and P25 photocatalysts in terms of toluene removals in a continuous flow reactor. The XPS measurement data indicated that the active N doping states exhibited N 1s binding energies were centered at 400 and 402 eV instead of the TiN binding at 396 eV commonly observed in the literature. The light absorption in the visible light range for N-doped TiO₂ was also confirmed by a clear red shift of the UV-visible spectra.     

Improved optical response and photocatalysis for N-doped titanium oxide (TiO2) films prepared by oxidation of TiN

In order to improve the photocatalytic activity, N-doped titanium oxide (TiO₂) films were obtained by thermal oxidation of TiN films, which were prepared on Ti substrates by ion beam assisted deposition (IBAD). The dominating rutile TiO₂ phase was found in films after thermal oxidation. According to the results of X-ray photoelectron spectroscopy (XPS), the residual N atoms occupied O-atom sites in TiO₂ lattice to form TiON bonds. UV-vis spectra revealed the N-doped TiO₂ film had a red shift of absorption edge. The maximum red shift was assigned to the sample annealed at 750 °C, with an onset wavelength at 600 nm. The onset wavelength corresponded to the photon energy of 2.05 eV, which was nearly 1.0 eV below the band gap of pure rutile TiO₂. The effect of nitrogen was responsible for the enhancement of photoactivity of N-doped TiO₂ films in the range of visible light.     

Enhanced visible light photocatalytic properties of Fe-doped TiO2 nanorod clusters and monodispersed nanoparticles

In order to get photocatalysts with desired morphologies and enhanced visible light responses, the Fe-doped TiO₂ nanorod clusters and monodispersed nanoparticles were prepared by modified hydrothermal and solvothermal method, respectively. The microstructures and morphologies of TiO₂ crystals can be controlled by restraining the hydrolytic reaction rates. The Fe-doped photocatalysts were characterized by X-ray diffraction (XRD), transmission electron microscopy (TEM), X-ray photoelectron spectroscopy (XPS), UV-vis absorption spectroscopy (UV-vis), N₂ adsorption-desorption measurement (BET), and photoluminescence spectroscopy (PL). The refinements of the microstructures and morphologies result in the enhancement of the specific surface areas. The Fe³⁺-dopants in TiO₂ lattices not only lead to the significantly extending of the optical responses from UV to visible region but also diminish the recombination rates of the electrons and holes. The photocatalytic activities were evaluated by photocatalytic decomposition of formaldehyde in air under visible light illumination. Compared with P25 (TiO₂) and N-doped TiO₂ nanoparticles, the Fe-doped photocatalysts show high photocatalytic activities under visible light.