H2分子在Mg3N2表面吸附的第一性原理研究

采用第一性原理方法,通过计算表面能确定Mg₃N₂（011）为最稳定的吸附表面,分别研究了H₂分子在Mg₃N₂（011）三种终止表面的吸附性质.研究发现H₂分子平行表面放置更有利于吸附,表面能最低的终止表面Model Ⅱ上吸附H₂分子最稳定,主要存在三种化学吸附方式：第一种吸附方式,H₂分子解离成2个H原子分别吸附在N原子上形成双NH基,这是最佳吸附方式;此时H₂分子与Mg₃N₂表面间主要是H原子的1s轨道和N原子的2s、2p轨道发生作用,N-H之间为典型的共价键.第二种吸附方式中H₂分子部分解离,两个H原子吸附在同一个N原子上形成NH₂基.第三种吸附方式中H₂分子解离成两个H原子,一个H原子和表面N原子作用形成NH基,另一个H原子和表面Mg原子作用形成MgH结构.三种吸附方式不存在竞争关系,形成双NH基的吸附方式反应能垒最低,最容易发生.除此之外H₂还能以分子的形式吸附在晶体表面,形成物理吸附.     

CO2在α-U(001)表面的吸附和解离

采用广义梯度密度泛函理论研究了0.25ML覆盖度下CO₂在α-U（001）表面上的吸附和解离,得到了CO₂的稳定吸附构型和吸附能,确定了CO₂的解离过渡态和解离能垒,探讨了CO₂与表面U原子的相互作用本质.结果表明CO₂趋向以C（O）-U多键结合方式在α-U（001）面发生强化学吸附,吸附能为1.24-1.67 eV;C-O键的活化程度依赖于表面电子向CO₂发生转移的程度.CO₂与表面U原子的相互作用主要来自于U原子电子向CO₂最低空轨道（LUMO）2π_u转移,以及CO₂π_u/1π_g/3σ_u-U 6d轨道间杂化而生成新的化学键.以形成3个C-U键和6个O-U键模式在穴位1和穴位2上发生吸附的CO₂（H1-C₃O₆和H2-C₃O₆）的解离吸附能分别为3.15和3.13 eV,解离能垒分别为0.26和0.36 eV,预示着吸附CO₂分于易于解离形成CO分子和O原子.     

二维金属-六亚氨基苯框架材料的气体吸附效应

利用密度泛函理论研究了气体分子(NH₃, H₂O, H₂S, NO₂)吸附在二维M₃(HIB)₂(M=Ni, Cu; HIB为六亚氨基苯)薄膜上体系的几何结构和电子结构的变化. 结果表明, 2种薄膜对气体分子的响应不同. 其中NH₃, H₂O和H₂S在M₃(HIB)₂薄膜表面的吸附较弱, 主要与薄膜的亚氨基形成氢键, 吸附能均小于-0.36 eV, 吸附对体系电子性质的影响很小. 但是 NO₂分子在薄膜表面形成化学吸附, 吸附能在-0.65~-1.72 eV范围内. 吸附NO₂分子使其电子结构发生明显改变, 如Cu₃(HIB)₂在费米能级处打开带隙, 由金属性质转变为半导体性质. 这是由于NO₂分子的p_z轨道与金属原子$d_{z}^{2}$ 轨道发生了强烈的轨道杂化. 此外, 研究发现高浓度的NO₂分子吸附能够使Ni₃(HIB)₂薄膜由非磁性变为磁性体系, 由普通金属性质变为半金属性质; 而高浓度的NO₂分子使Cu₃(HIB)₂薄膜由金属性质变为半导体性质, 薄膜电导率降低.     

利用原位APXPS与STM研究H2在ZnO(10${\rm{\bar 1}}$0)表面的活化

Cu/ZnO/Al₂O₃是工业中最广泛使用的甲醇合成催化剂。然而该催化反应的活性位点和机理目前仍存争议。H₂作为反应物之一,研究其在ZnO表面的活化和解离对于弄清甲醇合成反应的催化机理具有重要的帮助。本工作利用近常压光电子能谱(APXPS)和扫描隧道显微镜(STM)原位研究了H₂在ZnO(10${\rm{\bar 1}}$0)表面上的活化和解离。APXPS结果表明：在0.3 mbar (1 mbar = 100 Pa)的H₂气氛中,室温下ZnO表面形成羟基(OH)吸附物种。STM实验发现通入H₂后ZnO表面发生了(1×1)到(2×1)的重构。上述结果和原子H在ZnO(10${\rm{\bar 1}}$0)表面的吸附结果一致。然而吸附H₂O可以导致同样的现象。因此,我们还开展了H₂O在ZnO(10${\rm{\bar 1}}$0)表面吸附的对比实验。结果表明：H₂气氛中ZnO表面发生0.3 eV的能带弯曲,而H₂O吸附实验中几乎观察不到能带弯曲发生。同时,热稳定性实验表明H₂气氛中ZnO表面的OH不同于H₂O解离吸附产生的OH,前者具有更高的脱附温度。因此,本工作的结果表明常温和常压下H₂在ZnO(10${\rm{\bar 1}}$0)表面发生解离吸附。这一结果和以往超高真空下未发现H₂在ZnO(10${\rm{\bar 1}}$0)表面上的解离不同,说明H₂的活化是一个压力依赖过程。     

H2,C2H4在铂及铂锡合金上化学吸附的量子化学计算

本文详尽地分析了推广的休克尔分子轨道理论方法(EHMO)中参量化过程。借助于计算双原子体系选择出合理的经验参数和近似方式,引进了过渡金属内层原子轨道排斥作用项。分别计算了H,H₂,C₂H₄和C₂H₃在铂及铂锡合金上化学吸附键能,计算结果表明,同铂金属比较,在铂锡合金上H原子,C₂H₄分子的化学吸附键变弱在锡富集的铂锡合金上单个的铂原子不能解离吸附H₂分子,在铂锡合金上C₂H₄脱氢反应较难进行。     

Sc,Ti,V修饰B/N掺杂单缺陷石墨烯的储氢研究

3d过渡金属修饰是改善石墨烯储氢性能的最有效途径, 但仍存在金属团聚和H₂解离导致难以脱附的问题. 提出了B/N掺杂单缺陷石墨烯(BMG/NMG)的策略来避免以上两个问题. 密度泛函理论计算结果表明, N掺杂可以使Sc, Ti, V与石墨烯的结合能提高3~4倍, B掺杂可以将Sc与石墨烯的结合能提高3倍. Sc/BMG和Sc/NMG吸附的第一个H₂不会解离. Sc/BMG中Sc吸附5个H₂, 平均氢分子结合能为-0.18～-0.43 eV, 并且可以通过在同侧锚定多个Sc原子形成Sc/C₃B₂五元环增加H₂吸附位点. Sc/NMG中每个Sc吸附6个H₂, 平均氢分子结合能为-0.17～-0.29 eV, 还可以通过在异侧修饰形成Sc/N₃/Sc单元进一步提高储氢能力. 研究结果将为设计基于3d过渡金属修饰碳材料的储氢材料提供理论基础.     

化学链重整过程中LaFeO3载氧体的CH4部分氧化反应机理研究

本研究基于密度泛函理论(DFT)计算揭示了化学链重整过程中LaFeO₃载氧体的CH₄部分氧化反应机理,通过系统研究CH₄吸附活化、H₂和CO形成以及氧扩散等基元反应步骤,构建了CH₄部分氧化反应网络。研究发现,CH₄发生逐步脱氢反应形成H原子,其中,CH₃脱氢反应所需要克服的能垒(1.50 eV)最高,是CH₄逐步脱氢反应的限速步骤。载氧体表面H₂形成有两种路径,其中,H原子从O顶位迁移到Fe顶位,然后与另外O顶位的H原子成键形成H₂分子是主要途径。由于其相对较低的能垒(1.27 eV),CO的形成过程较易发生。氧扩散需要克服1.35 eV的能垒,表明氧扩散过程需要在高温下进行且扩散速率较低。通过比较各基元反应能垒,发现H₂形成是LaFeO₃载氧体CH₄部分氧化反应动力学的限速步骤,而H迁移是限制H     

H2分子在碱金属掺杂碳纳米管上的吸附特性

采用密度泛函理论研究了H₂在碱金属(M=Li, K)掺杂的扶手椅型单壁碳纳米管上的吸附. 对于碱金属管内掺杂, 模拟了4种氢吸附构型; 对于管外掺杂, 考虑了两种吸附结构, 同时还考虑了两种不同的掺杂浓度. 所有吸附模型都进行了全优化. 计算结果表明, 碱金属掺杂后, 碱金属与碳纳米管之间发生电子授受作用使得碱金属带正电荷, 对于金属Li, 管内掺杂更有利于电子向碳纳米管转移; 与管内掺杂相比, Li原子的管外掺杂更有利于H2分子吸附. 碱金属管外掺杂的碳纳米管吸附H₂的最稳定结构, 存在碱金属原子与H₂分子的配位作用.     

CO在α-U(001)表面的吸附

采用密度泛函理论中的广义梯度近似,计算了CO在α-U(001)表面的吸附、解离和扩散.结果表明:CO分子以CU3OU2构型化学吸附在α-U(001)表面,吸附能为1.78-1.99eV;吸附后表层U原子向上迁移,伴随着褶皱的产生;CO分子与表面U原子的相互作用主要是U原子的电子向CO分子最低空轨道2π*转移,以及CO2π*/5σ/1π-U6d轨道间杂化而生成新的化学键;CO解离吸附较分子吸附在能量上更为有利,h1(C)+h2(O)和h1(C)+h1(O)(h:空位)解离态吸附能分别为2.71和3.08eV;近邻三重穴位之间C、O原子的扩散能垒分别为0.57和0.14eV,预示O原子较C原子更易在U(001)表面扩散迁移.     

O_2在α-U(001)面吸附的密度泛函理论研究

采用广义梯度密度泛函理论结合周期性平板模型,计算了O2在α-U(001)表面吸附的几何和电子结构,并对H2、O2的吸附特性进行了对比分析。结果表明:O2分子在α-U(001)面上呈强解离化学吸附,吸附能为9.54～10.22eV,O-O距离较大的D+D-II构型最为稳定;吸附后表层U原子向上迁移,同时伴随着褶皱的产生;解离O原子与表面U原子的相互作用主要是离子键合,伴随着较弱的源于U5f/6d-O2p轨道杂化的共价键合;O原子的扩散能垒小于0.3eV,易于在U表面扩散迁移;O2分子在U表面的吸附强度较H2分子要大得多,对U表面结构的影响也更加显著。     

Li修饰B12N12储氢行为的密度泛函理论研究

采用基于密度泛函理论(DFT)的第一性原理投影缀加波方法, 研究了Li 修饰的B₁₂N₁₂笼子的储氢行为.计算结果表明: Li 原子吸附在B₁₂N₁₂笼子的四元环和六元环相交的B－N桥位上, 相对于其它六个高对称吸附位置更稳定, B₁₂N₁₂笼子周围最多可以吸附3 个Li 原子, 最稳定的构型是三个Li 原子同时吸附在N原子顶位(Top-N site). 每个Li 原子的周围能吸附三个氢分子, 笼子外侧还可以吸附两个氢分子, 内部最多可以吸附5 个氢分子. 考虑到笼内和笼外的吸附, B₁₂N₁₂笼子总的储氢量(氢分子)达到9.1% (w).     

Infrared spectroscopy of physisorbed and chemisorbed N2 in the Pt(111)(3x3)N2 structure

Using infrared spectroscopy and low electron energy diffraction, we have investigated the adsorption of N(2), at 30 K, on the Pt(111) and the Pt(111)(1x1)H surfaces. At monolayer coverage, N(2) orders in commensurate (3x3) structures on both surfaces, and we propose that the unit cells contain four molecules in each case. The infrared spectra reveal that N(2) exclusively physisorbs on the Pt(111)(1x1)H surface, while both physisorbed and chemisorbed N(2) is detected on the Pt(111) surface. Physisorbed N(2) is the majority species in the latter case, and the two adsorption states show an almost identical uptake behavior, which indicates that they are intrinsic constituents of the growing (3x3) N(2) islands. An analysis of the infrared absorbance data, based on a simple scaling concept suggested by density functional theory calculations, supports a model in which the (3x3) unit cell contains one chemisorbed molecule in end-on atop configuration and three physisorbed molecules. We note that a classic "pinwheel" structure on a hexagonal lattice, with the end-on chemisorbed N(2) molecules acting as "pins," is compatible with this composition.     

Pore with gate: enhancement of the isosteric heat of adsorption of dihydrogen via postsynthetic cation exchange in metal-organic frameworks

Three isostructural anionic frameworks {[(Hdma)(H(3)O)][In(2)(L(1))(2)]·4DMF·5H(2)O}(∞) (NOTT-206-solv), {[H(2)ppz][In(2)(L(2))(2)]·3.5DMF·5H(2)O}(∞) (NOTT-200-solv), and {[H(2)ppz][In(2)(L(3))(2)]·4DMF·5.5H(2)O}(∞) (NOTT-208-solv) (dma = dimethylamine; ppz = piperazine) each featuring organic countercations that selectively block the channels and act as pore gates have been prepared. The organic cations within the as-synthesized frameworks can be replaced by Li(+) ions to yield the corresponding Li(+)-containing frameworks {Li(1.2)(H(3)O)(0.8)[In(2)(L(1))(2)]·14H(2)O}(∞) (NOTT-207-solv), {Li(1.5)(H(3)O)(0.5)[In(2)(L(2))(2)]·11H(2)O}(∞) (NOTT-201-solv), and {Li(1.4)(H(3)O)(0.6)[In(2)(L(3))(2)]·4acetone·11H(2)O}(∞) (NOTT-209-solv) in which the pores are now unblocked. The desolvated framework materials NOTT-200a, NOTT-206a, and NOTT-208a display nonporous, hysteretic and reversible N(2) uptakes, respectively, while NOTT-206a and NOTT-200a provide a strong kinetic trap showing adsorption/desorption hysteresis with H(2). Single crystal X-ray analysis confirms that the Li(+) ions are either tetrahedrally (in NOTT-201-solv and NOTT-209-solv) or octahedrally (in NOTT-207-solv) coordinated by carboxylate oxygen atoms and/or water molecules. This is supported by (7)Li solid-state NMR spectroscopy. NOTT-209a, compared with NOTT-208a, shows a 31% enhancement in H(2) storage capacity coupled to a 38% increase in the isosteric heat of adsorption to 12 kJ/mol at zero coverage. Thus, by modulating the pore environment via postsynthetic cation exchange, the gas adsorption properties of the resultant MOF can be fine-tuned. This affords a methodology for the development of high capacity storage materials that may operate at more ambient temperatures.     

羟基磷灰石界面水行为的分子模拟

本文采用分子动力学模拟(MD)方法研究了羟基磷灰石(HAP)(001)和(100)晶面上的水分子行为，发现HAP晶面间的水是处在高电场和高内压的环境下，并可在晶面处形成2～3层高度结构化的水层，这些水具有有序结构和类冰固化特征。其中在HAP晶体的[001]方向具有较强的极性，相对于[100]方向能诱导产生更多的有序结构化水层。研究发现HAP-水界面处钙和磷酸根位点分布和水分子的吸附位点相关，并且水在HAP界面上的吸附形式具有多样性。该工作揭示了HAP界面结构化水层的形成及其结构细节特征。HAP晶面附近的结构化水层可阻止溶液离子自由出入晶面，对HAP颗粒在水溶液中的动力学稳定性具有重要的影响。     

水对锂交换低硅铝比八面沸石吸附性能的影响

研究了变压吸附空气分离制氧吸附剂——锂交换低硅铝比八面沸石LiLSX中残留水及从外部引入的水对吸附性能的影响.研究表明，在水合LiLSX经脱附后，当残留的水分子数目为0～32（个分子/晶胞）时， N2或O2的吸附量下降显著.原因是N2和O2的吸附主要依赖于处在SIII位置的32个锂离子.当水分子与SIII位置的Li＋结合时，就会阻碍N2或O2的吸附.而从外部引入的水分子与脱附残留的水分子相比，在相同水含量时对吸附量的影响较小，这是由于吸附位置的不均匀性以及水分子在沸石中的扩散行为所引起.在水扩散进入LiLSX内部的过程中，一部分水分子可以吸附在能量较低的位置上而不是吸附到最强的SIII位置上.     

Organoaluminium and -gallium compounds with N,N-diisopropylaminomethyl groups

The N,N-diisopropylaminomethyl aluminium compound [tBu2AlCH2NiPr2 x LiCl]2(1) and the gallium compounds Li[tBu2Ga(CH2NiPr2)2](2) and [tBu2GaCH2N(H)iPr2]Cl x tBu3Ga (3) were prepared by transmetallation of N,N-diisopropylaminomethyllithium LiCH2NiPr2 with di-tert-butylaluminium or -gallium chloride, and characterised by elemental analyses, multinuclear NMR spectroscopy (1H, 13C, 27Al, 7Li) and IR spectroscopy. The crystal structures have been determined by single crystal X-ray diffraction. Compound aggregates as a centrosymmetric dimer, with two Al-C-N units connected by a frame of two LiCl molecules [Al-Cl 2.367(1), Cl-Li 2.339(4) and 2.374(4), Li-N 1.977(4)A]. Compound 2 is a lithium organogallate with two weak LiN bonds [1.965(7) and 1.937(7)A]. Compound 3 contains two different moieties: tBu3Ga and a [tBu2GaCH2N(H)iPr2]+ cation, which are bridged by a Cl- anion [Ga-Cl 2.445(1) and 2.579(1), HCl 2.362(3)A].     

Adsorption and reaction of CO and CO2 on oxidized and reduced SrTiO3(100) surfaces

The adsorption and reaction of CO and CO(2) on oxidized and reduced SrTiO(3)(100) surfaces have been studied with temperature programmed desorption (TPD) and X-ray photoelectron spectroscopy (XPS). XPS results indicate that the oxidized SrTiO(3)(100) surfaces are nearly defect-free with predominantly Ti(4+) ions whereas the sputter-reduced surfaces contain substantial amounts of defects. Both CO and CO(2) are found to adsorb weakly on the oxidized SrTiO(3)(100) surfaces. On sputter-reduced surfaces, enhanced reactivity of CO and CO(2) is observed due to the presence of oxygen vacancy sites, which are responsible for dissociative adsorption of these molecules. Our studies indicate that the CO and CO(2) molecules exhibit relatively weaker interactions with SrTiO(3)(100) compared to those with TiO(2)(110) and TiO(2)(100) surfaces. This is most likely an influence of the Sr cations on the electronic structure of the Ti cations in the mixed oxide of SrTiO(3).     

Multiple Ionic-Covalent Couplings in Molecules and Clusters

The electronic states of molecules made of electropositive and electronegative components result from the interference between the covalent configurations and the ionic configurations. This work shows complex aspects of these ionic-covalent couplings in small molecules such as Li2H, Li2F, and Li4F. The extension of this type of analysis to the adsorption of the electrophilic molecules on the metal clusters or on the metal surfaces is supposed to lead to a radically new interpretation of the observed physical and chemical properties.     

Aggregation of donor base stabilized 2-thienyllithium in a single crystal and in solution: distances from X-ray diffraction and the nuclear Overhauser effect

Various 2-thienyllithium derivatives were investigated in the solid state by X-ray diffraction and in solution by 2D NMR experiments. The determined structures of [(Et(2)O)Li(C(4)H(3)S)](4) (1), [(THF)(2)Li(C(4)H(3)S)](2) (2), [(DME)Li(C(4)H(3)S)](2) (3), [(TMEDA)Li(C(4)H(3)S)](2) (4), and [(PMDETA)Li(C(4)H(3)S)] (5) (DME = 1,2-dimethoxyethane, TMEDA = N,N,N',N'-tetramethylethylene-1,2-diamine, and PMDETA = N,N,N',N",N"-pentamethyldiethylenetriamine) were solved in nondonating toluene and provide firm ground for diffusion-ordered NMR spectroscopy as well as heteronuclear Overhauser enhancement NMR spectroscopy. The distance relation of nuclear Overhauser effects with a factor of r(-6) is employed to gain further insight into the aggregation degree of 1-5 in solution. Comparison of the slope provided by the linear region of the buildup curves and of the ∑r(-6) calculated distances from the crystal structures offers a handle to judge the structure retention versus conversion in solution. The structures of 3-5 are maintained in toluene solution. The data of 2, however, indicate a partial dissociation or a rapid exchange between the vertices of a tetrameric core and free THF molecules. Auxiliary exchange spectroscopy investigations showed that the signals of the nitrogen donor base containing compounds 4 and 5 exchange with the signals of nonlithiated thiophene. This is explained by exchange of the deuterium by a hydrogen atom via lithiation of toluene molecules.     

H2分子在LaFeO3表面吸附的第一性原理研究

基于密度泛函理论的第一性原理方法,通过计算表面能确定LaFeO₃(010)表面为最稳定的吸附表面,研究了H₂分子在LaFeO₃(010)表面的吸附性质。LaFeO₃(010)表面存在LaO和FeO₂两种终止表面,但吸附主要发生在FeO₂终止表面,由于LaFeO₃(010)表面弛豫的影响,使得凹凸不平的表面层增加了表面原子与H原子的接触面积,表面晶胞的纵向体积增加约2.5%,有利于H原子向晶体内扩散。研究发现,H₂分子在LaFeO₃(010)表面主要存在3种化学吸附方式:第一种吸附发生在O-O桥位,2个H原子分别吸附在2个O原子上,形成2个-OH基,这是最佳吸附位置,此时H原子与表面O原子的作用主要是H1s与O2p轨道杂化作用的结果,H-O之间为典型的共价键。H₂分子的解离能垒为1.542 eV,说明表面需要一定的热条件,H₂分子才会发生解离吸附;第二种吸附发生在Fe-O桥位,1个H原子吸附在O原子上形成1个-OH基,另一个H原子吸附在Fe原子上形成金属键;第三种吸附发生在O顶位,2个H原子吸附在同一个O原子上,形成H₂O分子,此时H₂O分子与表面形成物理吸附,H₂O分子逃离表面后容易形成氧空位。此外,H₂分子在LaFeO₃(010)表面还可以发生物理吸附。