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1.
Density functional theory (DFT) calculations are conducted to explore the interaction of H2 with pure and Ti-doped WO3 (002) surfaces. Four top adsorption models of H2 on pure and Ti-doped WO3 (002) surfaces are investigated respectively, they are adsorption on bridging oxygen O1c, absorption on plane oxygen O2c, absorption on 5-fold W5c (Ti), and absorption on 6-fold W6c. The most stable and H2 possible adsorption structure in the pure surface is H-end oriented to the surface plane oxygen O2c site, while the favourable adsorption sites for H2 in a Ti-doped surface is not only an O2c site but also a W6c site. The adsorption energy, the Fermi energy level EF, and the electronic population are investigated and the H2-sensing mechanism of a pure-doped WO3 (002) surface is revealed theoretically: the theoretical results are in good accordance with our existing experimental results. By comparing the above three terms, it is found that Ti doping can obviously enhance the adsorption of H2. It can be predicted that the method of Ti-doped into a WO3 thin film is an effective way to improve WO3 sensor sensitivity to H2 gas.  相似文献   

2.
胡明  王巍丹  曾晶  秦玉香 《中国物理 B》2011,20(10):102101-102101
Density functional theory (DFT) calculations are employed to explore the NO2-sensing mechanisms of pure and Ti-doped WO3 (002) surfaces. When Ti is doped into the WO3 surface, two substitution models are considered: substitution of Ti for W6c and substitution of Ti for W5c. The results reveal that substitution of Ti for 5-fold W forms a stable doping structure, and doping induces some new electronic states in the band gap, which may lead to changes in the surface properties. Four top adsorption models of NO2 on pure and Ti-doped WO3 (002) surfaces are investigated: adsorptions on 5-fold W (Ti), on 6-fold W, on bridging oxygen, and on plane oxygen. The most stable and likely NO2 adsorption structures are both N-end oriented to the surface bridge oxygen O1c site. By comparing the adsorption energy and the electronic population, it is found that Ti doping can enhance the adsorption of NO2, which theoretically proves the experimental observation that Ti doping can greatly increase the WO3 gas sensor sensitivity to NO2 gas.  相似文献   

3.
Pure and WO3 doped CeO2-PbO-B2O3 glasses are prepared by the melt-quench technique. The structural and optical analyses of glasses are carried out by XRD, FTIR, density and UV-vis spectroscopic measurement techniques. FTIR analysis indicates the transformation of structural units of BO3 into BO4 with W-O-W vibration and the presence of WO4 and WO6 units observed with increase in WO3 contents. Decrease in band gap for CeO2-PbO-B2O3 glasses from 2.89 to 2.30 eV and for WO3 doped glasses from 2.89 to 1.95 eV has been observed and discussed. This decrease in band gap with WO3 doping approaches to semiconductor behavior. It shows that the presence of WO3 in the glass samples causes more compaction of the borate network due to the formation of BO4 groups and the presence of WO4 and WO6 groups, which result in a decrease in the optical band gap energy and increase in the density.  相似文献   

4.
Mine A. Gülmen 《Surface science》2006,600(21):4909-4921
The adsorption properties of CO on Pt3Sn were investigated by utilizing quantum mechanical calculations. The (1 1 1), (1 1 0) and (0 0 1) surfaces of Pt3Sn were generated with all possible bulk terminations, and on these terminations all types of active sites were determined. The adsorption energies and the geometries of the CO molecule at those sites were found. Those results were compared with the results obtained from the adsorption of CO on similar sites of Pt(1 1 1), Pt(1 1 0) and Pt(0 0 1) surfaces. The comparison reveals that adsorption of CO is stronger on Pt surfaces; this may be the reason why catalysts with Pt3Sn phase do not suffer from CO posioning in experimental works. Aiming to understand the interactions between CO and the metal adsorption sites in detail, the local density of states (LDOS) profiles were produced for atop-Pt adsorption, both for the carbon end of CO for its adsorbed and free states, and for the Pt atom of the binding site. LDOS profiles of C of free and adsorbed CO and Pt for corresponding pure Pt surfaces, Pt(1 1 1), Pt(1 1 0) and Pt(0 0 1) were also obtained. The comparison of the LDOS profiles of Pt atoms of atop adsorption sites on the same faces of bare Pt3Sn and Pt surfaces showed the effect of alloying with Sn on the electronic properties of Pt atoms. Comparison of LDOS profiles of the C end of CO in its free and atop adsorbed states on Pt3Sn and LDOS of Pt on bare and CO adsorbed Pt3Sn surface were used to clear out the electronic changes occurred on CO and Pt upon adsorption. The study showed that (i) inclusion of a Sn atom at the adsorption site structure causes dramatic decrease in stability which limits the number of possible CO adsorption sites on Pt3Sn surface, (ii) the presence of Sn causes angles different from 180° for M-C-O orientation, (iii) the presence of Sn in the neighborhood of Pt on which CO is adsorbed causes superposition of the 5σ/1π derived-state peaks at the carbon end of CO and changes in adsorption energy of CO, (iv) Sn present beneath the adsorption site strengthens the CO adsorption, whereas neighboring Sn on the surface weakens it for all Pt3Sn surfaces tested and (v) the most stable site for CO adsorption is the atop-Pt site of the mixed atom termination of Pt3Sn(1 1 0).  相似文献   

5.
陈玉红  杜瑞  张致龙  王伟超  张材荣  康龙  罗永春 《物理学报》2011,60(8):86801-086801
采用第一性原理方法研究了H2分子在Li3N(110)晶面的表面吸附. 通过研究H2/Li3N(110)体系的吸附位置、吸附能和电子结构发现: H2分子吸附在N桥位要比吸附在其他位置稳定,此时在Li3N(110)面形成两个-NH基,其吸附能为1.909 eV,属于强化学吸附;H2与Li3N(110)面的相互作用主要是H 1s轨道与N 关键词: 第一性原理 3N(110)')" href="#">Li3N(110) 2')" href="#">H2 吸附和解离  相似文献   

6.
First-principle calculations based on density function theory (DFT) are used to clarify the roles of γ-Fe2O3 in fly ash for removing mercury from coal-fired flue gases. In this study, the structure of key surface of γ-Fe2O3 is modeled and spin-polarized periodic boundary conditions with the partial relaxation of atom positions are employed. Binding energies of Hg on γ-Fe2O3 (0 0 1) perfect and defective surfaces are calculated for different adsorption sites and the potential adsorption sites are predicted. Additionally, electronic structure is examined to better understand the binding mechanism. It is found that mercury is preferably adsorbed on the bridge site of γ-Fe2O3 (0 0 1) perfect surface, with binding energy of −54.3 kJ/mol. The much stronger binding occurs at oxygen vacancy surface with binding energy of −134.6 kJ/mol. The calculations also show that the formation of hybridized orbital between Hg and Fe atom of γ-Fe2O3 (0 0 1) is responsible for the relatively strong interaction of mercury with the solid surface, which suggests that the presently described processes are all noncatalytic in nature. However, this is a reflection more of mercury's amalgamation ability.  相似文献   

7.
采用密度泛函理论和slab模型,研究NH3在Ni单原子层覆盖的Pt(111)和WC(001)表面上的物理与化学行为,计算了Ni单原子覆盖表面的电子结构以及NH3的吸附与分解.表面覆盖的单原子层中,Ni原子的性质与Ni(111)面上的Ni原子明显不同.与Ni(111)相比,Ni/Pt(111)和Ni/WC(001)表面上Ni原子dz2轨道上的电子更多地转移到了其它位置,该轨道上电荷密度降低有利于NH3吸附.在Ni/Pt(111)和Ni/WC(001)面上NH3吸附能均大于Ni(111),NH3分子第一个N-H键断裂的活化能则明显比Ni(111)面上低,有利于NH3的分解,吸附能增大使NH3在Ni/Pt(111)和Ni/WC(001)面上更倾向于分解,而不是脱附.N2分子的生成是NH3分解的速控步骤,该反应能垒较高,说明N2分子只有在较高温度下才能生成.WC与Pt性质相似,但Ni/Pt(111)和Ni/WC(001)的电子结构还是有差异的,与Ni(111)表面相比,NH3在Ni/Pt(111)表面上分解速控步骤的能垒降低,而在Ni/WC(001)上却升高.要获得活性好且便宜的催化剂,需要对Ni/WC(001)表面做进一步改进,降低N2分子生成步骤的活化能.  相似文献   

8.
利用X-射线光电子能谱(XPS)和程序升温脱附谱(TPD)研究了三甲基镓在Pd(111)表面的吸附和解离行为,并考察了表面预吸附H和O的影响。结果表明,在吸附温度为140 K时,三甲基镓在Pd(111)上主要为解离吸附,此时表面物种为Ga(CH3xx=1,2,3)和CHx物种。加热将导致Ga的甲基化合物中的Ga-C键发生分步断裂,在不同温度下产生CH4和H2从表面脱附。同时,XPS结果证实了在275~325 K的温度区间内存在Ga甲基化合物的分子脱附。退火至更高温度,表面只观察到积碳和金属Ga物种,这二者随着温度的继续升高逐渐向体相扩散。在Pd(111)表面预吸附O和H对上述吸附和解离行为存在显著的影响。当表面预吸附H时,脱附产物CH4和H2的脱附主要位于315 K,可归属为一甲基镓的解离脱附。当表面预吸附O时,只在258 K观察到CH4和H2的脱附峰,可能来自于Pd-O-Ga(CH32吸附结构的解离.  相似文献   

9.
TiO2 doped WO3 thin films were deposited onto glass substrates and fluorine doped tin oxide (FTO) coated conducting glass substrates, maintained at 500 °C by pyrolytic decomposition of adequate precursor solution. Equimolar ammonium tungstate ((NH4)2WO4) and titanyl acetyl acetonate (TiAcAc) solutions were mixed together at pH 9 in volume proportions and used as a precursor solution for the deposition of TiO2 doped WO3 thin films. Doping concentrations were varied between 4 and 38%. The effect of TiO2 doping concentration on structural, electrical and optical properties of TiO2 doped WO3 thin films were studied. Values of room temperature electrical resistivity, thermoelectric power and band gap energy (Eg) were estimated. The films with 38% TiO2 doping in WO3 exhibited lowest resistivity, n-type electrical conductivity and improved electrochromic performance among all the samples. The values of thermoelectric power (TEP) were in the range of 23-56 μV/K and the direct band gap energy varied between 2.72 and 2.86 eV.  相似文献   

10.
WO3 nanoparticles were prepared by evaporating tungsten filament under a low pressure of oxygen gas, namely, by a gas evaporation method. The crystal structure, morphology, and NO2 gas sensing properties of WO3 nanoparticles deposited under various oxygen pressures and annealed at different temperatures were investigated. The particles obtained were identified as monoclinic WO3. The particle size increased with increasing oxygen pressure and with increasing annealing temperature. The sensitivity increased with decreasing particle size, irrespective of the oxygen pressure during deposition and annealing temperature. The highest sensitivity of 4700 to NO2 at 1 ppm observed in this study was measured at a relatively low operating temperature of 50 °C; this sensitivity was observed for a sensor made of particles as small as 36 nm.  相似文献   

11.
Compared to experiment, the adsorption energies, bonding properties, and electronic structure of two different Al2O3/B4C bridge sites with seven different Al2O3 surfaces are investigated by ab initio periodic density functional theory. The Al2O3/B4C ceramic sintered in Ar is synthesized and measured by XRD and TEM. The calculated results reveal that the densification of O_bridge site of Al2O3/B4C surface is better than that of Al_bridge. The Al2O3 (1 1 3)/B4C with O_bridge is the most favorable and stable. The electronic structure shows that the electron hybridization exists between Al, O atoms and C, B atoms. The results indicate that the calculated results are in good agreement with the experiment.  相似文献   

12.
Lead bismuth arsenate glasses mixed with different concentrations of WO3 (ranging from 0 to 6.0 mol%) were synthesized. Differential thermal analysis (DTA), optical absorption, ESR and IR spectral studies have been carried out. The results of DTA have indicated that there is a gradual decrease in the resistance of the glass against devitrification with increase in the concentration of WO3 upto 4.0 mol%.The optical absorption spectra of these glasses exhibited a relatively broad band peaking at about 880 nm identified due to dxydx2y2 transition of W5+ ions; this band is observed to be more intense in the spectrum of glass containing 4.0 mol% of WO3. Further, two prominent kinks attributed to 3P01S0, 1D2 transitions of Bi3+ ions have also been located in the absorption spectra. The ESR spectra of these glasses recorded at room temperature exhibited an asymmetric signal at g∼1.71 and gll∼1.61. The intensity of the signal is observed to be maximal for the spectrum of the glass W4. The quantitative analysis of optical absorption and ESR spectral studies have indicated that there is a maximum reduction of tungsten ions from W6+ state to W5+ state in the glass containing 4.0 mol% of WO3. The IR spectral studies have indicated that there is a increasing degree of disorder in the glass network with increase in the concentration of WO3 upto 4.0 mol%.  相似文献   

13.
Y2O3:Eu3+ nanocrystals were prepared by combustion synthesis. The particle size estimated by X-ray powder diffraction (XRD) was about 10 nm. A blue-shift of the charge-transfer (CT) band in excitation spectra was observed in Y2O3:Eu3+ nanocrystals compared with bulk Y2O3:Eu3+. The electronic structure of Y2O3 is calculated by density functional method and exchange and correlation have been treated by the generalized gradient approximation (GGA) within the scheme due to Perdew-Burke-Ernzerhof (PBE). The calculated results show that the energy centroid of 5d orbital in nanocrystal has increasing trend compared with that in the bulk material. The bond length and bond covalency are calculated by chemical bond theory. The bond lengths of Y2O3:Eu3+ nanocrystal are shorter than those of the bulk counterpart and the bond covalency of Y2O3:Eu3+ nanocrystal also has an increasing trend. By combining centroid shift and crystal-field splitting, the blue-shift of the CT band is interpreted.  相似文献   

14.
Since the development of Scanning Tunnelling Microscopy (STM) technique, considerable attention has been devoted to various molecules adsorbed on various surfaces. Also, a new concept emerged with molecules on surfaces considered as nano machines by themselves. In this context, a thorough knowledge of surfaces and adsorbed molecules at an atomic scale are thus particularly invaluable. The present work describes the first Density Functional Theory (DFT) study of adsorption of CO, CO2 and NO molecules on a BaTiO3 surface following a first preliminary calculation of O and O2 adsorption on the same surface. In the previously considered work, we found that a (0 0 1) surface with BaO termination is more stable than the one with TiO2-termination. Consequently, we extended our study to CO, CO2 and NO molecules adsorbed on a (0 0 1) surface with BaO termination. The present calculation was performed on a (1 × 1) cell with one monolayer of adsorbed molecules. Especially, a series of cases implying CO molecules adsorbed in various geometrical configurations has been examined. The corresponding adsorption energy varies in the range of −0.17 to −0.10 eV. The adsorption energy of a CO2 molecule directly located above an O surface atom (called Os) is of the order of −0.18 eV. The O-C distance length is then 1.24 Å and the O-C-O and O-C-Os angles are 134.0° and 113.0°, respectively. For NO adsorption, the most important induced structural changes are the followings: (i) the N-O bond is broken when a NO molecule is absorbed on a Ba-Os bridge site. In that case, N and O atoms are located above an O and a Ba surface atom, respectively, whereas the O-Ba-Os and N-Os-Ba angles are 106.5° and 63.0°, respectively. The N-O distance is as large as 2.58 Å and the adsorption energy is as much as −2.28 eV. (ii) In the second stable position, the NO molecule has its N atom adsorbed above an Os atom, the N-O axis being tilted toward the Ba atom. The N-Os-Ba angle is then 41.1° while the adsorption energy is only −0.10 eV. At last, the local densities of states around C, O as well as N atoms of the considered adsorbed molecules have also been discussed.  相似文献   

15.
Thermal stability, interfacial structures and electrical properties of amorphous (La2O3)0.5(SiO2)0.5 (LSO) films deposited by using pulsed laser deposition (PLD) on Si (1 0 0) and NH3 nitrided Si (1 0 0) substrates were comparatively investigated. The LSO films keep the amorphous state up to a high annealing temperature of 900 °C. HRTEM observations and XPS analyses showed that the surface nitridation of silicon wafer using NH3 can result in the formation of the passivation layer, which effectively suppresses the excessive growth of the interfacial layer between LSO film and silicon wafer after high-temperature annealing process. The Pt/LSO/nitrided Si capacitors annealed at high temperature exhibit smaller CET and EOT, a less flatband voltage shift, a negligible hysteresis loop, a smaller equivalent dielectric charge density, and a much lower gate leakage current density as compared with that of the Pt/LSO/Si capacitors without Si surface nitridation.  相似文献   

16.
At the generalized gradient approximation (GGA), the elastic constants of the orthorhombic phase of NH3BH3 were calculated with plane-wave pseudo-potential method. Our calculation showed that the orthorhombic phase NH3BH3 is a loose and brittle material, as well as hard to be deformed, also we calculated the elastic anisotropies and the Debye temperatures from the elastic constants. And from the band structure and density of state (DOS), we concluded that NH3BH3 is a wide-gap semiconductor and the band gap is almost 6.0 eV. The bonds between N atoms and H atoms show a strong covalent characteristic, B atoms and H atoms form ironic bonds, and so as to the B-N bonds. Electrons from the B atoms are absorbed by the H atoms around the B atoms, and the H atoms display electronegativity.  相似文献   

17.
The adsorption of CO molecule on the O2 pre-adsorbed LaFeO3 (0 1 0) surface has been investigated using a density functional theory calculation. The calculated results show that the most appropriate reaction occurs between the CO and the pre-adsorbed O2. After CO adsorption, the bonding mechanism between Fe site and the pre-adsorbed O2 is not modified, and the HOMO–LUMO energy gap of the M1 mode is narrowed, which is caused by the redistribution of electron density in the surface.  相似文献   

18.
磁控溅射法制备的CaCu3Ti4O12薄膜   总被引:2,自引:0,他引:2       下载免费PDF全文
周小莉  杜丕一 《物理学报》2005,54(4):1809-1813
采用溅射方法成功地制备了CaCu33Ti44O1212薄膜, 用原子力显微镜、x射线衍射(XRD)仪和LCR分析仪对样品进行形貌、物相结构和介电性质的研究.XRD表明,薄膜比块体的晶 格常数小但晶格畸变较大;LCR测量结果显示,在相同温度下薄膜比块体的相对介电常数低 ,薄膜相对介电常数由低到高转变时对应的温度较高且激活能较大.分析表明:薄膜的相对 介电常数较低是样品中晶相含量较低、缺陷较多使内部阻挡层电容大量减小、致密度不高引 起的;薄膜中 关键词: 磁控溅射 3Ti44O1212')" href="#">CaCu33Ti44O1212 介电常 数 激活能  相似文献   

19.
BaO oxide is the main storage component of the NOx storage and reduction catalysts. Herein, the interactions between the NO2 molecule and the unsupported as well as γ-Al2O3 supported BaO clusters have been studied using the first principle density functional theory calculation. Our results indicated that there is a strong synergetic effect involving both the BaO clusters and the surface of the γ-Al2O3 substrate toward NO2 adsorption. The interfacial region between the monodispersed BaO cluster and the substrate surface that allows NO2 to bond with the cluster and the surface simultaneously was shown to be optimal for NO2 adsorption.  相似文献   

20.
祝国梁  疏达  戴永兵  王俊  孙宝德 《物理学报》2009,58(13):210-S215
采用基于密度泛函理论的第一性原理方法,研究了Si原子在TiAl3中的格点取代行为.通过对不同原子被置换后的c/a值、形成能以及电子态密度的计算和比较,发现Si原子倾向于取代TiAl3中的Al原子,其取代行为主要由系统的电子结构决定,计算结果与实验相符.为了进一步研究Si原子的取代行为,对Si原子占据的格点以松散或紧凑分布下体系的总能、形成能以及电子态密度进行了计算,结果表明Si原子倾向于取代TiAl3中松散分布的Al(2)原子.对c/a值的计算表明,随Al(2)格点Si原子浓度的增加,c/a值逐渐增大;而当Si取代Al(1)格点时,c/a值随Si原子浓度的增加而减小.研究表明,Si在TiAl3中的极限固溶度介于12.5at%—18.75at%之间. 关键词: 密度泛函理论 第一性原理 电子结构 3')" href="#">TiAl3  相似文献   

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