H_2O分子在锐钛矿型TiO_2(101)表面的吸附特性与微观机理

本文采用基于密度泛函理论(DFT)的平面波超软赝势方法,模拟计算H2O分子在锐钛矿型TiO2(101)无氧空位和有氧空位表面的吸附行为,对吸附能、吸附距离、吸附前后表面电子态密度以及光学性质分别进行分析,结果表明:H2O分子在无氧空位锐钛矿型TiO2(101)表面不容易被吸附,在含有氧空位缺陷的表面容易被吸附;稳定吸附后,H2O分子平面垂直于TiO2表面;负电中心(O端)距空位越近,吸附越稳定,且氧空位浓度越高,吸附效果越明显;通过电子态密度分析发现,H2O分子吸附于含氧空位的表面后,由于H2O分子中O原子的2p孤对电子掺入,新峰值在费米能级附近出现,提高了材料在可见光低能区域的跃迁几率,明显改善了对可见光的吸收系数和反射率,光学气敏传感特性显著.     

H2O分子在锐钛矿型TiO2(101)表面的吸附特性与微观机理

近年来,随着着光纤技术和光集成技术的发展,光学气敏湿度传感器被广泛应用,在气敏传感材料领域中,由于TiO2具有灵敏度高、响应时间快等优点而受到广泛关注。本文采用基于密度泛函理论(DFT)的平面波超软赝势方法,模拟计算H2O分子在锐钛矿型TiO2(101)无氧空位和有氧空位表面的吸附行为,对吸附能、吸附距离、吸附前后表面电子态密度以及光学性质分别进行分析,结果表明：H2O分子在无氧空位锐钛矿型TiO2(101)表面不容易被吸附,在含有氧空位缺陷的表面容易被吸附;稳定吸附后,H2O分子平面垂直于TiO2表面;负电中心（O端）距空位越近,吸附越稳定,且氧空位浓度越高,吸附效果越明显;通过电子态密度分析发现,H2O分子吸附于含氧空位的表面后,由于H2O分子中O原子的2p孤对电子掺入,在费米能级附近出现新峰值,提高了材料在可见光低能区域的跃迁几率,明显改善了对可见光的吸收系数和反射率,光学气敏传感特性显著。     

First-principles study on anatase TiO2（101） surface adsorption of NO

In this paper, the stable structure and the electronic and optical properties of nitric oxide （NO） adsorption on the anatase TiO2 （101） surface are studied using the plane-wave ultrasoft pseudopotential method, which is based on the density functional theory. NO adsorption on the surface is weak when the outermost layer terminates on twofold coordinated oxygen atoms, but it is remarkably enhanced on the surface containing O vacancy defects. The higher the concentration of oxygen vacancy defects, the stronger the adsorption is. The adsorption energies are 3.4528 eV （N end adsorption）, 2.6770 eV （O end adsorption）, and 4.1437 eV （horizontal adsorption）. The adsorption process is exothermic, resulting in a more stable adsorption structure. Furthermore, O vacancy defects on the TiO2 （101） surface significantly contribute to the absorption of visible light in a relatively low-energy region. A new absorption peak in the low-energy region, corresponding to an energy of 0.9 eV, is observed. However, the TiO2 （101） surface structure exhibits weak absorption in the low-energy region of visible light after NO adsorption.     

Fe~(3+)-Doped Anatase TiO_2 Study Prepared by New Sol-Gel Precursors

FeTi_1-O_2(= 0.00,0.05,0.10) nanocomposites are synthesized using a sol-gel method involving an ethanol solvent in the presence of ethylene glycol as the stabilizer,and acetic acid as the chemical reagent.Their structural and optical analyses are studied to reveal their physicochemical properties.Using the x-ray diffractometer(XRD)analysis,the size of the nanoparticles(NPs) is found to be 18–32 nm,where the size of the NPs decreases down to 18 nm when Fe impurity of up to 10% is added,whereas their structure remains unchanged.The results also indicate that the structure of the NPs is tetragonal in the anatase phase.The Fourier transform infrared spectroscopy analysis suggests the presence of a vibration bond(Ti–O) in the sample.The photoluminescence analysis indicates that the diffusion of Fe~(3+) ions into the TiO_2 matrix results in a decreasing electron–hole recombination,and increases the photocatalytic properties,where the best efficiency appears at an impurity of10%.The UV-diffuse reflection spectroscopy analysis indicates that with the elevation of iron impurity,the band gap value decreases from 3.47 eV for the pure sample to 2.95 eV for the 10 mol% Fe-doped TiO_2 NPs.     

甲醇分子在金红石TiO2(110)和锐钛矿TiO2(001)表面吸附和反应的活性位点

通过高分辨的扫描隧道显微术研究并比较了金红石型TiO₂(110)-(1×1)和锐钛矿型TiO₂(001)-(1×4)两种表面的活性位点． 在金红石型TiO₂(110)-(1×1)表面, 观察到氧空位缺陷是O₂和CO₂分子的活性吸附位点,而五配位的Ti原子是水分子和甲醇分子的光催化反应活性位点．在锐钛矿型TiO₂(001)-(1×4)表面,观察到完全氧化的表面,Ti原子更可能是六配位的,H₂O和O₂分子均不易在这些Ti原子上吸附．经还原后表面出现富Ti的缺陷位点, 这些缺陷位点对H₂O和O₂分子表现出明显的活性． 锐钛矿型TiO₂(001)-(1×4)表面的吸附和反应活性并不具有很高的活性,某种程度上其表现出的活性似乎低于金红石型TiO₂(110)-(1×1)表面．     

Adsorption of 1,3,5-Triphenylbenzene Molecules and Growth of Graphene Nanoflakes on Cu(100) Surface

Adsorption of 1,3,5-triphenylbenzene(TPB) molecules on Cu( 100) surface is studied using ultraviolet photoelectron spectroscopy(UPS) and density functional theory(DFT) calculations. Researches on the bottom-up fabrication of graphene nanoflakes(GNFs) with TPB as a precursor on the Cu(100) surface are carried out based on UPS and DFT calculations. Three emission features d, e and f originating from the TPB molecules are located at 3.095, 7.326 and 9.349 eV below the Fermi level, respectively. With the increase of TPB coverage on the Cu(100) substrate, the work function decreases due to the formation of inter facial dipoles and charge(electron)rearrangement at the TPB/Cu(100) interface. Upon the formation of GNFs, five emission characteristic peaks of g, h, i, j and k originating from the GNFs are located at 1.100, 3.529, 6.984, 8.465 and 9.606 eV below the Fermi level, respectively. Angle resolved ultraviolet photoelectron spectroscopy(ARUPS) and DFT calculations indicate that TPB molecules adopt a lying-down configuration with their molecular plane nearly parallel to the Cu(100) substrate at the monolayer stage. At the same time, the lying-down configuration for the GNFs on the Cu(100) surface is also unveiled by ARUPS and DFT calculations.     

密度泛函理论方法研究6H-SiC(0001)表面对氧分子和水分子的吸附

本文通过密度泛函方法计算6H-SiC(0001)表面对氧分子和水分子的吸附. 在6H-SiC(0001)表面上吸附的O₂分子自发地解离成O^*,并被吸收在C与Si原子之间的空位上. 吸附的H₂O自发地分解成OH^*和H^*,它们都被吸附在Si原子的顶部,OH^*进一步可逆地转化为O^*和H^*. H^*可以使Si悬键饱和并改变O^*的吸附类型,并进一步稳定6H-SiC(0001)表面并防止其转变为SiO₂.     

Nickel Adsorption on Bi2Se3 Surface

Physics of the Solid State - The effect of the physical adsorption of nickel on a surface of a topological Bi2Se3 insulator on the electronic structure has been studied. The influence of the...     

氢分子在Mg2Ni(010)面的吸附与分解

本文采用基于密度泛函理论(DFT)的第一原理赝势平面波(PW-PP)方法,对氢分子在Mg2Ni(010)面的吸附与分解进行了研究,我们发现氢分子以Hor1的方式吸附在表面层Ni原子的顶位时吸附能最高,为0.6769eV,这表明氢分子最可能以Hor1的方式吸附在表面层Ni原子的顶位,此时氢分子跟表面的距离( )和氢分子的键长( )分别为1.6286Å和0.9174Å. 在分子吸附的基础上计算了氢分子沿着选取的反应路径分解时的反应势垒,发现要使氢分子分解需要0.2778eV的活化能,而氢分子分解时的吸附能为0.8390eV,分解后两个氢原子的距离为3.1712Å. 在分子吸附和分解吸附时氢原子跟正下方的Ni原子都有较强的相互作用,氢原子所得到的电子主要来自氢分子正下方的Ni原子.     

Dependence of Nonlinear Optical Response of Anatase TiO_2 on Shape and Excitation Intensity

Nonlinear optical(NLO) properties of anatase TiO_2 with nanostructures of nanoparticle(NP), nanowire(NW)and annealed nanowire(NWA) are studied by open-aperture and closed-aperture Z-scan techniques with a femtosecond pulsed laser at wavelengths of 532 nm and 780 nm simultaneously. At 532 nm,when increasing excitation intensity, NLO absorption of TiO_2 NPs transforms from saturable absorption to reverse-saturable absorption.However, NWs and NWAs exhibit the opposite change. At 780 nm,all samples show reverse-saturable absorption, but have different sensitivities to excitation intensity Due to the larger surface-to-volume ratio of NPs and less defects of NWAs by annealing, nonlinear optical absorption coefficients follow the order NPs≥NWs≥NWs.The results also show that these shape and annealing effects are dominant at low excitation intensity but do not exhibit at the high excitation intensity. The NLO refractive index of NPs shows a positive linear relationship with the excitation intensity whereas NW and NWAs exhibit a negative linear relationship.The results could provide some foundational guidance to applications of anatase TiO_2 in optoelectronic devices or other aspects.     

第一性原理研究H_2O分子在CaCO_3(104)表面吸附

基于密度泛函理论的第一性原理方法模拟研究H_2O在CaCO_3(104)表面的吸附特征.首先,研究H_2O分子在CaCO_3(104)表面的顶位、桥位(短桥位、长桥位)和穴位上垂直和平行表面两种类型下的8种高对称吸附结构模型,结合吸附能和稳定吸附构象确定最优吸附位.而后,基于H_2O/CaCO_3(104)最优吸附结构模型,研究吸附前后H_2O和CaCO_3(104)表面的物理结构、电子结构(Mulliken电荷布居数、态密度、电子局域函数)的特征,分析H_2O/CaCO_3(104)表面之间的相互作用以及成键机理.研究结果:吸附能和体系稳定构象显示H_2O分子/CaCO_3(104)表面的最稳定吸附结构为穴位-平行.在穴位-平行位吸附后,H_2O分子的O-H键长和H-O-H键角均发生改变; CaCO_3晶体平行和垂直(104)表面方向上原子位置均发生改变,表面层变化最大;即吸附作用对H_2O分子和CaCO_3晶体的物理结构均产生较大影响; H_2O/CaCO3(104)最优吸附体系的Mulliken电荷布居数、电子态密度、电子局域函数的研究均说明H_2O分子与CaCO3(104)之间存在电子的转移形成化学键.其中,Ca-O(H_2O)形成离子键,H(H_2O)-O(CaCO_3)之间存在氢键作用.本文研究揭示了方解石表面水湿性的原因,同时为方解石润湿性的深入研究奠定基础.     

Adsorption of Fe on GaAs(100) Surface

The adsorption of one monolayer Fe atoms on an ideal GaAs (100) surface is studied by using the self-consistent tight-binding linear muffin-tin orbital method. The Fe adatom chemisorption on Ga- and As-terminatedsurface are considered separately. A monolayer of S atoms is used to saturate the dangling bonds on one of the supercellsurfaces. Energies of adsorption systems of an Fe atom on different sites are calculated, and the charge transfers areinvestigated. It is found that Fe-As interaction is stronger than Fe-Ga interaction and Fe atoms prefer to be adsorbed onthe As-terminated surface. It is possible for the adsorbed Fe atoms to sit below the As-terminated surface resulting inan Fe-Ga-As mixed layer. The layer projected density states are calculated and compared with that of the clean surface.     

Van der Waals Epitaxy of Anatase TiO_2 on mica and Its Application as Buffer Layer

MICAtronics, based on the functional oxide/mica heterostructures, has recently attracted much attention due to its potential applications in transparent, flexible electronics and devices. However, the weak van der Waals interaction decreases the tolerable lattice mismatch and thus limits the species of function oxides that are able to be epitaxially grown on mica. We successfully fabricate relatively high-quality epitaxial anatase TiO_2 thin films on mica substrates. Structural analyses reveal that the carefully chosen growth temperature(650℃) and suitable crystalline phase(anatase phase) of TiO_2 are the key issues for this van der Waals epitaxy. Moreover, as a buffer layer, the TiO_2 layer successfully suppresses the decomposition of BiFeO_3 and the difficulty of epitaxial growth of BiFeO_3 is decreased. Therefore, relatively high-quality anatase TiO_2 is proved to be an effective buffer layer for fabricating more functional oxides on mica.     

两种不同极性有机小分子在方解石(104)面吸附的密度泛函研究

利用密度泛函理论研究苯甲酸和甲苯两种不同极性的有机小分子在方解石（104）面的吸附特征，分析极性对有机小分子吸附的影响.结果表明：苯甲酸趋向于以分子态、单齿吸附模式倾斜吸附于方解石（104）面，吸附能为-1.394 eV；甲苯平行吸附于方解石（104）面，吸附能为-0.362 eV.有机小分子吸附于方解石（104）面过程中体系的几何结构和电子结构发生明显变化.苯甲酸分子几何结构变化幅度远大于甲苯.苯甲酸与方解石（104）面之间形成Ca-O离子键和H-O共价键，甲苯与方解石（104）面之间仅存在微弱的氢键相互作用.苯甲酸和甲苯等两种不同极性有机小分子在方解石（104）面的吸附特征和吸附机理存在较大的差异，苯甲酸分子的吸附强度远高于甲苯.本文揭示了不同极性有机小分子在方解石（104）面的吸附机理，为提高油藏采收率和矿物浮选等工程问题提供理论依据.     

臭氧在SnO2表面吸附的红外光谱研究

以SnO2催化臭氧化降解高浓度糖蜜酒精废水为探针反应,研究SnO2催化臭氧化降解糖蜜酒精废水的活性,并采用红外光谱研究臭氧在SnO2及金属氧化物改性的SnO2催化剂表面的吸附行为。结果表明:由纯氧源制得的O3在SnO2表面吸附的红外光谱上的1 027和1 055 cm-1及2 099和2 122 cm-1处存在两处明显的吸收双峰,而空气制备的O3在SnO2表面与CO及CO2等存在竞争吸附,使得O3的吸附减少,催化臭氧化降解糖蜜废水的降解率下降。催化剂助剂对SnO2催化臭氧化降解糖蜜酒精废水有较大的影响。采用Fe2O3,NiO,CuO,ZnO,MgO,SrO及BaO等金属氧化物为助剂改性的SnO2在2 236和2 213 cm-1,1628和1 599 cm-1出现强度相似的吸收峰,但是几种催化剂对CO2和CO的吸附差别较大,过渡金属改性的SnO2在1 580~1 070 cm-1处出现较宽的吸收峰,碱土金属氧化物改性的SnO2催化剂在1 580~1 070 cm-1之间,出现了1 298和1 274 cm-1两个新的峰,从而引起了不同助剂催化臭氧化的活性差别,碱土金属改性的SnO2对糖蜜酒精废水的催化臭氧化脱色效果明显优于过渡金属改性的SnO2,其中BaO改性的SnO2催化剂的活性最好。     

NH_x(x=1～3)在金属Ir表面吸附与解离的第一性原理研究

采用密度泛函理论,在slab模型下,研究了NH_x(x=1~3)在Ir(100)、Ir(111)和Ir(110)表面上的最稳定吸附位置、几何构型以及逐步脱氢分解过程,计算了相应的吸附能和活化能.计算结果表明,在Ir(100)、Ir(111)面上,NH_3是以C_3轴垂直吸附在顶位,在Ir(110)上,NH_3是以N-Ir键与表面成68.6°吸附在顶位,且吸附能依赖于表面的结构而不同,相比而言,NH_3更容易吸附在开放表面Ir(100)、Ir(110)面上,说明NH_3在这些表面的吸附具有结构敏感性.NH_(x(x=1~3))的分解,在Ir(100),NH_3的吸附与分解存在竞争,在Ir(110)面NH_3最容易分解,在Ir(111)面NH_3是分子性吸附,不能分解.NH_2、NH在三个表面均能够分解,在Ir(110)面活化能均较高.     

Ru(0001)表面氮分子和钡原子的相互作用

本文采用密度泛函理论方法研究了Ru(0001)表面氮分子和钡原子的相互作用。计算结果表明,钡原子的作用弱化了氮分子键。氮分子键长从Ru(001)-N2表面的0.113 nm伸长至Ru(001)-N2/Ba表面的0.120 nm;分子的拉伸振动频率从2221 cm-1减小到1746 cm-1;氮分子得到的电荷数从清洁表面的0.3 e增加到1.1 e。电荷从钡原子6s轨道向钌原子4d轨道转移,转移电荷增强了氮分子 空轨道和钌原子4d轨道间的杂化作用,导致 分子轨道和 杂化轨道发生极化。轨道极化使分子电偶极矩增加了约-0.136 eÅ。金属钡在Ru(0001)表面氮分子活化过程中具备电子型助催剂的特征。     

碳吸附于Fe（100）表面的第一性原理研究

本文采用自旋极化密度泛函理论计算了清洁Fe（100）表面及C吸附于Fe（100）表面三种结构: p(2×2)、c(2×2)及p(2×1)。清洁Fe(001)表面只有弛豫,没有重构。吸附C原子的Fe表面体系,最稳定位置为四重空位,空位吸附的C原子实际上与Fe成五重键,这与实验相符。通过对c(2×2)表面结构的电子态密度计算,发现C原子的s、p态与表面Fe原子的d、p及s态都有不同程度的相互作用,成键的主要作用为C2p态与Fe3dx2-y2、3dxy 态的杂化。     

洁净和氧吸附的Cu(100)表面重构的理论研究

在密度泛函理论下,计算了清洁和吸附氧原子的Cu(100)表面的驰豫和优势吸附构型。结果表明,氧原子在金属表面采用四重穴位时,具有最大的结合能,顶位吸附时结合能最小,桥位吸附时结合能居间。这一计算结果与实验报道一致。各种密度泛函方法的比较后,发现采用mPW1PW91密度泛函和LanL2dz赝势基组,能够准确给出与实验相符的计算结果。平板模型计算的分态密度图显示,在吸附过程中出现d轨道向Fermi能级移动并越过Fermi能级,而O原子的p轨道能级远离Fermi能级,表明有电子从铜原子的d轨道转移到氧原子的2p轨道,簇模型和平板模型的布居分析显示表面氧带有约0.65～0.7 e的负电荷。研究表明,采用适当的基组和泛函方法,即使采用簇模型来模拟表面,也可以获得与实验比较吻合的计算结果。