非晶硅短程序与电子结构关系的量子化学研究

本支通过对Si_(29)无规网络原子簇模型的CNDO计算,探讨了非晶硅(a-Si)结构短程序对其电子态密度(DOS)分布的影响。结果表明,在与实验原子径向分布函数(RDF)基本相同的条件下,a-Si模型中的键角和二面角是影响电子态密度分布的主要参数。     

径向分布函数法及其在研究高聚物结构中的应用(4)

图谱解释我们曾讨论过非晶高聚物的径向分布函数(RDF)的基础理论,并指出用规范化的实验数据处理和误差修正方法能获得可靠的RDF,本文讨论对它的解释。由RDF曲线中峰的位置,可求出相对某一参考原子邻近的最大电子密度,亦即相对参     

疏水改性聚丙烯酰胺溶液的分子模拟

设计了几种不同的非离子型改性聚丙烯酰胺(HM-PAM)和阴离子型改性聚丙烯酰胺(HM-HPAM). 通过分子动力学模拟(MD)方法研究了在聚合物链上加入不同疏水改性单体对提高聚丙烯酰胺耐盐性的影响, 考察了盐浓度对疏水改性聚丙烯酰胺的回旋半径(R_g)、 特性黏数([η])、 径向分布函数(RDF)和均方位移(MSD)的影响以及聚合物的微观结构与特性黏数之间的关系. 研究结果表明, 引入疏水改性单体后, 改性聚丙烯酰胺具有较好的耐盐性. 通过研究非键作用与氢键相互作用可知, 体系中溶质和溶剂间的相互作用及氢键作用越弱, 溶液的特性黏数越大. O-H原子对的RDF结果表明, 聚合物链的伸展与聚合物链及官能团间的相互作用有关. 当RDF峰较弱时, 聚合物链与水的作用越弱, 越有利于聚合物链保持舒展状态, 溶液的特性黏数也就越大. 另外, 从聚合物链的MSD曲线发现, 聚合链的移动性与特性黏数呈负相关.     

水、甲醇和乙醇液体微结构性质的Car-Parrinello 分子动力学模拟

采用Car-Parrinello 分子动力学(CPMD)方法分别研究了水、甲醇和乙醇的液体微结构性质.研究结果显示:在水、甲醇和乙醇三个体系中O…O径向分布函数曲线的第一个峰位置分别为0.278、0.276 和0.275nm; O…H径向分布函数曲线的第一个峰位置分别为0.178、0.176和0.177 nm.表明基团(氢原子、甲基、乙基)的差异对O…O第一个峰的位置影响很小.但基团的差异对径向分布函数峰高的影响却很显著,由水到乙醇第一个峰的高度逐渐变高.空间分布函数表明氧原子和氢原子在溶剂分子周围有取向地分布,这与径向分布函数所表现出尖锐的第一个峰相一致.氢键分布分析显示,水、甲醇和乙醇的平均氢键数分别为3.62、1.99 和1.87,表明水形成了网状氢键结构,而甲醇、乙醇形成链状氢键结构.     

铯在叶蜡石孔隙中吸附与扩散的分子动力学研究

本文采用分子动力学方法(molecular dynamics, MD)模拟研究了Cs~+在叶蜡石纳米孔隙中的吸附和扩散行为.径向分布函数和配位数的分析表明,在叶蜡石孔隙中Cs~+的第一水合壳层半径为3.05?,水合数为8.0～8.5.原子密度分布表明Cs~+是以外层表面络合物的形式吸附在叶蜡石基面上. Cs~+的水合结构及其吸附百分比受浓度和温度的影响均较小.随着温度升高, Cs~+热运动加剧导致其扩散系数显著增大.     

“拟双子”阴离子表面活性剂在癸烷/水界面的分子动力学模拟

采用全原子分子动力学模拟方法研究了壬基酚取代的系列烷基磺酸盐表面活性剂在癸烷/水界面的微观聚集行为,通过分析界面厚度、界面生成能和界面张力以及表面活性剂分子与水分子之间的径向分布函数和配位数,讨论了不同磺烷基链长度对壬基酚基取代烷基磺酸盐表面活性剂界面性质的影响.结果表明,磺烷基链长为12时,表面活性剂的界面张力最低,界面厚度和界面生成能最大.     

PET薄膜非晶区结构的RDF研究

本文将在低角度范围应用的X射线衍射计算机分峰法扩展到含所有非晶峰的广角度范围,用分离的广角度非晶散射导出径向分布函数(RDF);并通过对取向产生的附加分布函数分析,研究了成膜过程聚对苯二甲酸乙二醇脂(PET)膜非晶区结构的变化。     

剪应力下弱作用势胶体颗粒聚团的特点

探讨了不同剪应力下，具有Ｌｅｎｎａｒｄ－Ｊｏｎｅｓ势的胶体颗粒聚团的结构特性，包括簇团的大小分布，径向分布函数，分形维数和原子配位数。研究表明，在弱作用力下，胶体簇团的分布随剪应力的增加而趋向小簇团一边；径向分布函数曲线随剪应力的增加而降低，胡在近程距离内降低得最多；分形维数随剪应力的增加表现为先增加后减小的趋势，其值随模拟条件的不同而在１．９－２．４之间变动。剪应力“场”对分形维数的大小没有太大     

电子衍射径向分布函数测定稀土顺1,4聚丁二烯的原子间距分布

本文用电子衍射径向分布函数测定了稀土顺1,4聚丁二烯的原子间距分布。从电子衍射实验强度曲线的傅里叶变换得到的RDF曲线上,具有二个分子内峰和三个分子间峰。说明在熔点以上,处于非晶态的顺1,4聚丁二烯中不同程度的存在分子链间的局部有序性。     

二十面体准晶对非晶形成影响的模拟

采用分子动力学模拟技术,以液态金属Ni为例,研究了在不同冷却条件下形成晶体及非晶的过程.模拟采用镶嵌原子法(EAM)作用势,得到了不同温度、不同冷却速度下Ni的径向分布函数以及原子组态变化的重要信息,利用键对分析技术探讨了二十面体准晶对非晶形成的影响.     

X-ray photoelectron spectroscopy and first principles calculation of BCN nanotubes

Multiwalled boron carbonitride (BCN) nanotubes with two different structures were synthesized via thermal chemical vapor deposition; one has 10% C atoms homogeneously doped into BN nanotubes (B0.45C0.1N0.45 NTs), and the other has BN layers sheathed with 5-nm-thick C outerlayers (BN-C NTs). The electronic structures of the B, C, and N atoms were thoroughly probed by synchrotron X-ray photoelectron spectroscopy and the X-ray absorption near-edge structure method. The B0.45C0.1N0.45 NTs contain a significant amount of B-C and C-N bonding with a pyridine-like structure (hole structure), which reduces the pi bonding states of the B and N atoms. From the XPS valence band spectrum, the band gap was estimated to be about 2.8 eV. In the BN-C NTs, the C and BN domains are separated without forming the pyridine-like structure. Using the first principles method, we investigated the relative stabilities and electronic structures of the various isomers of the double-walled (12,0)@(20,0) BCN NTs. The C-outerlayer BN nanotube structure is the most stable isomer, when there exist no defects in the tubes with B/N = 1.0 (i.e., graphite-like structure). In addition, a reasonable model, which is characterized by the motives consisted of three pyridine-like rings around a hollow site, is presented for the local structure of C atoms in the B0.45N0.45C0.1 NTs. A considerable decrease of the band gap due to the 10% C doping was predicted, which was consistent with the experimental results.     

RADIAL DISTRIBUTION FUNCTION OF cis-1,4-POLYBUTADIENE BY ELECTRON DIFFRACTION

The interatomic distance function of rareearth catalyzed cis-1,4-polybutadiene was studied by" radial distribution function (RDF) derived from electron diffraction. Two intramolecular peaks and three interrnolecular peaks have been found on the RDF. The appearance of such a number of intermolecular maxima on the RDF can be explained by the local parallel packing of long molecular chains of the amorphous polymers.     

RDF法对非晶态聚醚砜共聚物的近程有序结构研究

用径向分布函数(RDF)研究了聚醚砜共聚物(PES)在r=1.5 nm范围内的近程结构, 结果表明, 分子链间存在近程有序结构, 有序周期约为0.5 nm; 聚醚砜共聚物经退火处理后, 由g(r)图可以看出, 第一个峰变高、变窄; 由G(r)图可以看出, 分子链间第一个有序区内, 分子链间贡献大于链内贡献; 于200 ℃退火处理后有序畴尺寸(rs)略有增大, 原子平均位移(σ)变小, 使得分子链内原子间距分布更加均匀, 相邻分子链间距(rv)变小. 同时透射电镜(TEM)的形态结构分析表明, 经退火处理后, 其聚集态确实形成了某种局部有序的结构.     

Surface Chemistry and Catalytic Reactivity of Borocarbonitride in Oxidative Dehydrogenation of Propane

Borocarbonitride (BCN) materials are newly developed oxidative dehydrogenation catalysts that can efficiently convert alkanes to alkenes. However, BCN materials tend to form bulky B₂O₃ due to over-oxidation at the high reaction temperature, resulting in significant deactivation. Here, we report a series of super stable BCN nanosheets for the oxidative dehydrogenation of propane (ODHP) reaction. The catalytic performance of the BCN nanosheets can be easily regulated by changing the guanine dosage. The control experiment and structural characterization indicate that the introduction of a suitable amount of carbon could prevent the formation of excessive B₂O₃ from BCN materials and maintain the 2D skeleton at a high temperature of 520 °C. The best-performing catalyst BCN exhibits 81.9 % selectivity towards olefins with a stable propane conversion of 35.8 %, and the propene productivity reaches 16.2 mmol h⁻¹ g⁻¹, which is much better than hexagonal BN (h-BN) catalysts. Density functional theory calculation results show that the presence of dispersed rather than aggregated carbon atoms can significantly affect the electronic microenvironment of h-BN, thereby boosting the catalytic activity of BCN.     

Prepeak in the structural factor. Inhomogeneous packings of Lennard-Jones atoms

This work reports on the effects of structural inhomogeneities within the models of spherical atomic packings on the radial distribution function (RDF) and the structural factor (SF). Models of inhomogeneous packings were constructed by removing some atoms from homogeneous packing according to a predetermined template. Thus various additional voids, leading to specific structural correlations of atoms on a middle scale (several atomic sizes), are introduced in the model. A dense noncrystalline packing of 27,000 Lennard-Jones atoms serves as the initial system. Three various templates were used, and models containing different fractions of additional voids were constructed with each of these templates. It is demonstrated that RDF is only slightly sensitive to such inhomogeneities; in contrast, the SF has additional peaks at small q, these peaks being notable even after removal of a small fraction of atoms. Some models yield a single narrow prepeak, which is akin to that observed in diffraction experiment for some glasses.     

Fe68Si32合金液态结构与固态组织的相关性

利用液态X射线衍射仪研究了Fe68Si32合金的液态结构，获得了结构因子、径向分布函数、原子间的最近邻距离和配位数.结果表明，在1250～1450 ℃范围内液态合金的最近邻距离为0.259～0.260 nm，配位数为10.3(±0.2)；液态合金的结构因子在Q=15.5 nm－1处有一明显的预峰存在.根据预峰的特性，建立了Fe68Si32熔体的结构模型，即体心立方结构的有序Fe3Si原子团以共面的方式形成Fe3Si面心立方超结构(DO3)；合金在1250 ℃的径向分布函数的Gauss分解结果与合金的面心立方模型吻合较好.预峰的产生是面心立方超结构原子团中Si原子之间相互关联的外在表现. Fe68Si32合金的固态X射线衍射显示合金中含有Fe3Si相，而且其特征峰与合金的结构因子的峰位基本一致，表明Fe68Si32合金的液固态结构之间联系紧密.     

Possible mechanism of BN fullerene formation from a boron cluster: Density‐functional tight‐binding molecular dynamics simulations

We simulate the formation of a BN fullerene from an amorphous B cluster at 2000 K by quantum mechanical molecular dynamics based on the density‐functional tight‐binding method. We run 30 trajectories 200 ps in length, where N atoms are supplied around the target cluster, which is initially an amorphous B₃₆ cluster. Most of the incident N atoms are promptly incorporated into the target cluster to form B‐N‐B bridges or NB₃ pyramidal local substructures. BN fullerene formation is initiated by alternating BN ring condensation. Spontaneous atomic rearrangement and N₂ dissociation lead to the construction of an sp² single‐shelled structure, during which the BN cluster undergoes a transition from a liquid‐like to a solid‐like state. Continual atomic rearrangement and sporadic N₂ dissociation decrease the number of defective rings in the BN cluster and increase the number of six‐membered rings, forming a more regular shell structure. The number of four‐membered rings tends to remain constant, and contributes to more ordered isolated‐tetragon‐rule ring placement. © 2016 Wiley Periodicals, Inc.     

Some cluster and condensed-phase properties of light elements: B to P

Attention is first drawn to disordered condensed phases of Si and C. Amorphous Si, with clear-cut tetrahedral coordination, is treated by combining sp³ hybridization with a random network model of structure, X-ray and electron diffraction experiments confirm both electron density and structural models. Recent work using the Car-Parrinello technique is then reviewed, with the aim of comparing and contrasting amorphous C and Si and their liquid phases. After a brief review of the structure and bonding in clusters of Al and P atoms, some results on clusters of Na are presented and related to cohesion in the condensed metallic phase. Then, fission of doubly charged Na clusters is treated at some length and, in particular, is related to quantum chemical procedures. A short summary concerning π-bands in graphitic and boron nitride layers is followed by a discussion of BN alternants, both buckytubes and octahedral symmetry cages being considered, along with C analogs. © 1997 John Wiley & Sons, Inc. Int J Quant Chem 63: 695–707, 1997     

BCN化合物的合成与表征

以石墨和六方氮化硼(h-BN)粉为原料,利用高能机械球磨和高温高压技术对BCN化合物的形成、结构及相变进行了研究.经120h球磨制备出BCN非晶体.在1400cm^-1附近,BCN非晶有一宽化的强红外吸收峰,在740和1630cm^-1附近观察到弱的红外吸收峰;在1330cm^-1附近观察到一宽化的Raman散射峰.BCN非晶中B_1s的结合能为191.9eV,C_1s的结合能为284.9和286.8eV,N_1s的结合能为398.3和400.5eV.将BCN非晶在4GPa和1473K下退火45min后转化为六方结构的BCN晶体,其晶格常数为a=0.2505nm,c=0.6664nm.其红外光谱特征吸收峰分别出现在1398,1103,1024,925和802cm^-1.Raman散射峰分别出现在1328,1358,1582和1614cm^-1.并对非晶BCN的形成和相转变机制进行了研究.