CO在SnO2(110)面吸附特性的密度泛函研究

根据密度泛函理论, 采用广义密度近似和总体能量平面波赝势方法, 以6层Slab周期结构为模型, 计算了CO以4种不同方式在SnO2(110)表面的吸附, 研究了CO吸附对表面特性的影响. 计算结果表明, CO以C端向下在低配位Sn5C位置的顶位吸附为稳定的吸附方式, 该吸附对表面的驰豫现象有所改善. CO吸附并未明显改变表面电子态密度分布, 但造成了费米能1.06 eV的升高. 吸附后CO分子向表面转移了0.07个电子, 使表面电阻下降. 理论计算的结果支持了气体传感器气敏机理中的表面电导模型.     

CO分子在不同类型Al2O3表面的吸附构型和电子结构

采用基于赝势平面波基组的密度泛函理论方法对CO分子在α-Al₂O₃（0001）以及γ-Al₂O₃的（100）、（110C）、（110D）表面上的吸附构型和电子结构进行系统研究.计算结果表明,CO倾向于选取C端吸附在表层Al原子上,并主要通过其5σ轨道与表面发生作用,吸附后部分电子从CO转移到底物,导致各Al₂O₃表面功函均发生不同程度的下降,与气相相比,吸附后CO分子的C-O伸缩振动频率均发生蓝移.通过对比CO在各表面上的吸附情况,可以看出CO可作为检测Al₂O₂不同类型表面活性中心的有效探针分子.     

一氧化碳分子在Pt/t-ZrO2(101)表面的吸附性质

运用广义梯度密度泛函理论(GGA-PW91)结合周期平板模型方法,研究了CO分子在完整与Pt负载的四方ZrO2(101)表面的吸附行为.结果表明:表面第二层第二氧位和表面第二桥位分别为CO分子和Pt原子在完整ZrO2(101)表面的稳定吸附位,且覆盖度为0.25ML(monolayer)时均为稳定吸附构型,吸附能分别为56.2和352.7kJ·mol-1.CO分子在负载表面的稳定吸附模式为C-end吸附,吸附能为323.8kJ·mol-1.考察了CO分子在负载表面吸附前后的振动频率、态密度和轨道电荷布居分析,并与CO分子和Pt原子在ZrO2表面的结果进行比较.结果表明,C端吸附CO分子键长为0.1161nm,与自由的和吸附在ZrO2表面后的CO相应值(0.1141和0.1136nm)相比伸长.吸附后C―O键伸缩振动频率为2018cm-1,与自由CO分子相比发生红移;吸附后CO带部分正电荷,电子转移以Pt5dCO2π的π反馈机理占主导地位.     

甲醇在活性Al2O3催化剂表面的吸附与脱水反应

 采用X射线衍射、红外光谱、程序升温脱附和微反等技术对一系列不同方法制备的活性Al2O3催化剂的结构和性能进行了表征,探讨了催化剂的结构与甲醇脱水反应性能之间的构效关系,提出了甲醇在活性Al2O3催化剂表面脱水的反应机理. 结果表明,活性Al2O3主要由γ-Al2O3和无定形的Al2O3组成,其表面存在σⅠ和σⅡ两种L酸吸附位. 甲醇在Al2O3表面有两种吸附态,即分子吸附态和解离吸附态,其中甲醇的分子吸附为可逆吸附,而解离吸附态甲醇(即甲氧基)在催化剂表面解离成表面甲氧基和羟基,当反应温度较高时,表面甲氧基会进一步分解产生CO,H2以及少量的CO2,CH4和C等. 二甲醚的生成是分子吸附态甲醇与临近的解离吸附态甲醇相互作用的结果.     

簇模型ZnO(100)面上吸附CO_2的密度泛函理论研究

采用电荷自洽方法, 以嵌入原子簇Zn4O4为模型, 使用量子化学的密度泛函理论, 研究了二氧化碳在六方ZnO非极化的(1010)面的可能吸附态。计算表明, CO2垂直底物表面吸附, 氧原子只能与Zn原子配位, 并且吸附能为很弱的1.8 kJ/mol;吸附质分子平行于底物表面时, 得到了5种平衡吸附构型, 其中采用CZn配位和η2O, O二齿配位时, 吸附很弱, 经BSSE校正后的吸附能在8.8~6.6 kJ/mol。 采用η2C, O方式分别与O和Zn配位时, 吸附能为31.1 kJ/mol; C原子与表面O配位时计算得到了唯一的一个化学吸附态, 吸附能为139.6 kJ/mol, 与实验结果一致。     

CO在δ-Pu(111)面吸附行为的周期性密度泛函理论研究

利用量子化学中的密度泛函理论结合周期模型方法研究了CO分子在δ-Pu(111)面的吸附行为.通过对不同吸附位置的吸附能和平衡几何结构比较发现,CO分子在δ-Pu(111)面的吸附C端吸附比O端吸附更有利,属于较强的化学作用,最稳定的吸附方式为心式垂直吸附,桥式次之,顶式最不稳定.心式垂直吸附的吸附能为-1.236 eV,C原子吸附位距离Pu表面0.212 2 nm,C-O键长0.120 8 nm.CO与Pu配位数目是决定化学吸附的主要因素,配位的Pu原子数目越多,化学成键越稳定.Mulliken电荷分析表明CO和Pu表面的作用主要发生在第一层,另外两层几乎没有影响.     

基于密度泛函理论计算的CO2在SrTiO3(100)表面的吸附

通过密度泛函理论的第一性原理,模拟了CO2分子在SrTiO3(100)表面TiO2-和SrO-位点上的吸附行为,获得了CO2在几种不同吸附模型下的结构参数及表面吸附能,进而研究了吸附机理和结构稳定性.计算结果表明,当CO2的C原子吸附在SrTiO3(100)表面SrO-及TiO2-位点的氧原子上时,吸附结构较稳定,尤其是C、O原子共吸附在TiO2-位点时最稳定,而其余吸附模型则不稳定.对吸附稳定模型的Mulliken布局数及态密度分析显示:CO2分子在SrTiO3(100)表面吸附主要是由于SrTiO3(100)面的电子跃迁至CO2分子,CO2分子得到电子形成弯曲的CO2-阴离子结构,并伴随着C-O键的伸长,从而达到吸附活化CO2的目的.     

TiO_2纳米膜上吸附态甲基橙的光催化降解反应活性研究

以反胶束溶液不同陈化是间及涂膜次数制备了三种TiO_2纳米膜,用XRD,SEM 和AFM方法考察了这些膜的形态结构特征,以吸附态甲基橙为模型反应物,研究 TiO_2纳米膜的光催化降解活性,并以AM1分子模拟计算探讨了甲基橙分子在不同膜 上可能的吸附态,及其与光催化降解的关联。结果表明,膜A最薄,膜上纳米粒子 分布均匀,表面平滑,甲基橙分子可能主要以端基方式吸附,这种吸附对分子骨架 化学键的影响较小,且不利于表面羟基对底物分子的进攻,结果反应活性低。膜B 最厚,对光的透过率最低,膜上纳米粒子分布很不均匀,表面缺陷结构丰富,对甲 基橙的吸附强,甲基橙分子主要以平卧式吸附,从而削弱了分子中的N=N双键,有 利于表面痉基对底物分子的进攻,光催化反应活性最高。膜C的厚度和粒子分布的 均匀性介于膜A和膜B之间,甲基橙分子可以两种方式吸附光催化反应的活性介于膜 A和膜B之间。     

TiO_2纳米膜上吸附态甲基橙的光催化降解反应活性研究

以反胶束溶液不同陈化是间及涂膜次数制备了三种TiO_2纳米膜，用XRD，SEM 和AFM方法考察了这些膜的形态结构特征，以吸附态甲基橙为模型反应物，研究 TiO_2纳米膜的光催化降解活性，并以AM1分子模拟计算探讨了甲基橙分子在不同膜 上可能的吸附态，及其与光催化降解的关联。结果表明，膜A最薄，膜上纳米粒子 分布均匀，表面平滑，甲基橙分子可能主要以端基方式吸附，这种吸附对分子骨架 化学键的影响较小，且不利于表面羟基对底物分子的进攻，结果反应活性低。膜B 最厚，对光的透过率最低，膜上纳米粒子分布很不均匀，表面缺陷结构丰富，对甲 基橙的吸附强，甲基橙分子主要以平卧式吸附，从而削弱了分子中的N=N双键，有 利于表面痉基对底物分子的进攻，光催化反应活性最高。膜C的厚度和粒子分布的 均匀性介于膜A和膜B之间，甲基橙分子可以两种方式吸附光催化反应的活性介于膜 A和膜B之间。     

簇模型ZnO(10(1-)0)面上吸附CO2的密度泛函理论研究

采用电荷自洽方法,以嵌入原子簇Zn4O4为模型,使用量子化学的密度泛函理论,研究了二氧化碳在六方ZnO非极化的(101^-0)面的可能吸附态。计算表明,CO2垂直底物表面吸附,氧原子只能与Zn原子配位,并且吸附能为很弱的1．8kJ／mol;吸附质分子平行于底物表面时,得到了5种平衡吸附构型,其中采用C-Zn配位和η^2-O,O二齿配位时,吸附很弱,经BSSE校正后的吸附能在8．8～6．6kJ／mol。采用η^2-C,O方式分别与O和Zn配位时,吸附能为31．1kJ／mol;C原子与表面O配位时计算得到了唯一的一个化学吸附态,吸附能为139．6kJ/mol,与实验结果一致。     

Dissociative adsorption of carbon monoxide on Mo(110): first-principles theory

The adsorption and dissociation of carbon monoxide on Mo (110) surface is studied with density functional theory. The results at different sites (atop, short bridge, long bridge, and hollow) are presented. The hollow site is found to be the most stable adsorption site for CO. The CO molecule is found to adsorb in end-on configurations (alpha states) at high coverage and inclined configurations (beta states) at low coverage. The dissociation activation energy from beta states is found to be approximately 1 eV lower than from alpha state. The adsorption of dissociation products, C and O, on Mo(110) has also been studied. The most stable adsorption site for C and O is long bridge and hollow site, respectively. The adsorption of C and O at low coverage is, in general, stronger than at high coverage, which is partly responsible for the high reactivity of CO dissociation at low coverage, since the binding energy of CO is not very sensitive to the coverage.     

NiO表面磁性对分子吸附的影响的第一性原理研究

过渡金属氧化物广泛应用在当今能源与环境相关的催化领域,理解其表面化学性质以及结构-反应活性之间的关系对于先进催化材料的进一步发展以至理性设计至关重要.3d后过渡系金属(Mn,Fe,Co,Ni)的氧化物以其中金属离子独特的自旋状态和由此产生的铁磁/反铁磁性为典型特征.研究过渡金属氧化物的自旋状态以及磁性对表面化学的影响将使我们更加完整了解这些材料的表面化学.以NiO为代表的后过渡系金属岩盐结构一元氧化物具有反铁磁性,被经常作为反铁磁研究的模型体系.尽管在低温(低于其Neel温度)下NiO体相的完整晶体具有确定的反铁磁序,但是一系列最新研究表明,在条件变化时NiO表面的Ni离子可以产生不同的磁序.以此为背景,本工作以NiO为模型体系,采用DFT+U的第一性原理方法研究了NiO表面磁序对表面的小分子吸附活性的影响,包括表面吸附活性对各磁性相的表面取向以及吸附物种磁性的依赖关系.我们考察了NiO的5种反铁磁相和一种铁磁相,两个晶面NiO(001)和NiO(011),顺磁性分子NO和非顺磁性分子CO.我们发现表面能受磁性的影响较轻微,NiO(001)面上从49到54 meV/?2,NiO(011)面上从162到172 meV/?2.在NiO(001)面上,CO与NO都倾向于在Ni离子的顶位吸附.对于不同的体相磁序与表面取向,CO吸附能的变化范围为-0.33~-0.37 eV,NO吸附能的变化范围为-0.42~-0.46 eV.在NiO(011)表面,两种分子都倾向于吸附在由两个Ni离子构成的桥位.我们发现相对于NiO不同磁性相的体相长程磁序,吸附位点处构成桥位的两个Ni离子的局部磁矩相对取向对于分子的吸附具有更加显著的影响.计算得到NO在局部磁矩相对取向反平行(↑↓)吸附位点处的吸附能为-0.99~-1.05 eV,在局部磁矩相对取向平行(↑↑)吸附位点处吸附会增强,吸附能为-1.21~-1.30 eV.对于CO,尽管计算的吸附能在(↑↓)吸附位点(-0.73~-0.75 eV)与在(↑↑)吸附位点(-0.71~-0.72 eV)非常接近,两种吸附位点处的CO吸附时分子轨道杂化方式以及吸附后CO的局域电子态密度却具有明显不同的特征.本工作突出揭示了分子在过渡金属氧化物表面的多重吸附位点上吸附时吸附位点的局域磁矩相对取向对吸附性能的影响.     

First-principles Periodic Density Functional Study of CO Adsorption on Spinel-type CuCr2O4 (100) Surface

The catalytic properties of CuCr2O4 with the cubic normal spinel-type structure were discussed by means of studying CO adsorption on the CuCr2O4 (100) surface in the framework of density functional theory. The results of geometry optimization show that CO prefers to adsorb at a Cu site with the adsorption energy of 133.2 kJ/mol. The adsorptions at all sites lead to a decrease in C-O stretching frequency, an increase in C-O bond length and a net positive Mulliken charge for the CO molecule. Population analysis indicates that the charges transfer from the CO molecule to substrate. The density of states for CO molecule before and after adsorption are also computed to discuss the bonding mechanism of CO.     

甲酸在Pt-Sn(111)/C合金表面吸附的量子化学研究

采用周期平板模型, 结合密度泛函理论对HCOOH和CO在Pt-Sn(111)/C表面的top、brigde、hcp和fcc共计8个位点的吸附模型进行构型优化和能量计算, 并对吸附前后的频率、电荷、能带和态密度进行了研究. 计算结果表明fcc-Pt₃是较为有利的吸附位点, Sn掺杂之后费米能级右移, 导带增宽, 价带和导带的位置略微降低, 合金表面电子结构变化利于甲酸的吸附解离催化, 可使甲酸燃料电池阳极催化性能显著提高. 通过催化剂表面的抗中毒分析, 发现CO在Pt-Sn(111)/C表面的吸附能以两种趋势下降, 阳极催化剂掺杂改性后抗CO中毒能力增强.     

A DFT study of the adsorption and dissociation of CO on Fe(100): influence of surface coverage on the nature of accessible adsorption states.

In the present article, we report adsorption energies, structures, and vibrational frequencies of CO on Fe(100) for several adsorption states and at three surface coverages. We have performed a full analysis of the vibrational frequencies of CO, thus determining what structures are stable adsorption states and characterizing the transition-state structure for CO dissociation. We have calculated the activation energy of dissociation of CO at 0.25 ML (ML = monolayers) as well as at 0.5 ML; we have studied the dissociation at 0.5 ML to quantify the destabilization effect on the CO(alpha3) molecules when a neighboring CO molecule dissociates. In addition, it is shown that the number and nature of likely adsorption states is coverage dependent. Evidence is presented that shows that the CO molecule adsorbs on Fe(100) at fourfold hollow sites with the molecular axis tilted away from the surface normal by 51.0 degrees. The asorprton energy of the CO molecule is -2.54 eV and the C-O stretching frequency is 1156 cm(-1). This adsorption state corresponds to the alpha3 molecular desorption state reported in temperature programmed desorption (TPD) experiments. However, the activation energy of dissociation of CO(alpha3) molecules at 0.25 ML is only 1.11 eV (approximately 25.60 kcal mol(-1)) and the gain in energy is -1.17 eV; thus, the dissociation of CO is largely favored at low coverages. The activation energy of dissociation of CO at 0.5 ML is 1.18 eV (approximately 27.21 kcal mol(-1)), very similar to that calculated at 0.25 ML. However, the dissociation reaction at 0.5 ML is slightly endothermic, with a total change in energy of 0.10 eV Consequently, molecular adsorption is stabilized with respect to CO dissociation when the CO coverage is increased from 0.25 to 0.5 ML.     

Titanium-decorated graphene oxide for carbon monoxide capture and separation

We propose titanium-decorated graphene oxide (Ti-GO) as an ideal sorbent for carbon monoxide (CO) capture and separation from gas mixtures. Based on first-principles calculations, Ti-GO exhibits a large binding energy of ~70 kJ mol(-1) for CO molecules, while the binding energies for other gases, such as N(2), CO(2), and CH(4), are significantly smaller. The gas adsorption properties of Ti-GO are independent of the local GO structures once Ti atoms are anchored by the oxygen-containing groups on the GO surface. The strong interaction between CO molecule and Ti is a result of dative bonding, i.e., hybridization between an empty d orbital of Ti and an occupied p orbital of CO. Adsorption isotherms from grand canonical Monte Carlo simulations clearly demonstrate the strong selectivity of Ti-GO for CO adsorption in a mixture with other gas.     

First principles study of adsorption and dissociation of CO on W(111)

The adsorption and dissociation of carbon monoxide on the W(111) surface is studied with density functional theory. The CO molecule is found to adsorb in end-on configurations (alpha states) and inclined configurations (beta states). The dissociation of the most strongly bound beta state CO is found to have an activation energy of about 0.8 eV, which is lower than the energy required to desorb CO molecularly from the surface. The diffusion of CO and O on W(111) is predicted to be facile at room temperature, whereas C atoms are virtually immobile up to approximately 600 K, according to our calculations. Preadsorbed carbon atoms are shown to prevent the dissociation of CO by blocking the most strongly bound beta state adsorption site and by blocking the dissociation pathway. We predict that dissociation of CO on W(111) is a self-poisoning process.     

CO2 adsorption on TiO2(101) anatase: a dispersion-corrected density functional theory study

Adsorption, diffusion, and dissociation of CO(2) on the anatase (101) surface were investigated using dispersion-corrected density functional theory. On the oxidized surface several different local minima were identified of which the most stable corresponds to a CO(2) molecule adsorbed at a five-fold coordinated Ti site in a tilted configuration. Surface diffusion is characterized by relatively small activation barriers. Preferential diffusion takes place along Ti rows and involves a cartwheel type of motion. The presence of a bridging oxygen defect or a surface interstitial Ti atom allows creation of several new strong binding configurations the most stable of which have bent CO(2) structures with simultaneous bonding to two surface Ti atoms. Subsurface oxygen vacancy or interstitial Ti defects are found to enhance the bonding of CO(2) molecules to the surface. CO(2) dissociation from these defect sites is calculated to be exothermic with barriers less than 21 kcal/mol. The use of such defects for catalytic activation of CO(2) on anatase (101) surface would require a mechanism for their regeneration.     

First‐Principles Study toward CO Adsorption on Au/Ni Surface Alloys

The introduction of a second metal, gold, into a nickel matrix can effectively improve the catalytic performance and thermal stability of the catalysts toward steam reforming of methane. To investigate the effect of Au on the adsorption properties and electronic structure of the Ni(111) surface, we chose CO as a probe molecule and examined CO adsorption on various Au/Ni surfaces. It was revealed that Au addition weakened the absorbate–substrate interactions on the Ni(111) surface. With increasing gold concentration, the binding energy declines further. The variation of the binding energies has been interpreted by exploring the electronic structure of surface nickel atoms. The effect of gold can be quantitatively characterized by the slopes of the fitting equations between the binding energy and the number of gold atoms surrounding the adsorption site. Our results show that the binding energy at top sites can be approximately estimated by counting the number of surrounding gold atoms. On one specific surface, the relative magnitude of the binding energy can be simply judged by the distance between gold and the geometrical center of the adsorption site. This empirical rule holds true for C, H, and O adsorption on the Au/Ni surface. It may be applicable to a system in which a doped atom of larger atomic size is incorporated into the host metal surface by forming a surface alloy.