吡啶团簇的飞秒光电离和从头计算研究

用飞秒激光电离飞行时间质谱研究了吡啶分子团簇在 4 0 0nm波长下的多光子光电离 ,实验观测到一系列的质子化和非质子化团簇离子 .结果表明 ,质子转移也能发生在弱氢键结合的分子间 .通过分析离子峰宽和离子信号强度随气源压力的变化 ,得到质子化团簇离子来源于大团簇离子的碎裂 ,而非质子化团簇离子是中性团簇直接电离的结果 .从头计算结果表明 ,吡啶团簇是通过弱氢键C -H…N结合在一起的 ,并且团簇离子离解倾向于生成质子化产物     

吡啶-水团簇(C_5H_5N)_n(H_2O)_m(n=1～2,m=1～4)结构和红外光谱的理论研究

利用密度泛函理论,在B3LYP/6-311++G(d,p)基组水平上对吡啶-水团簇(C5H5N)n(H2O)m(n=1~2,m=1~4)的可能构型进行全优化,得到了团簇的稳定结构;计算结果显示,在吡啶和水的二聚体中,稳定构型只有一种,没有发现通过π氢键(O—H…π)作用形成的团簇结构。为了研究各团簇结构的稳定性,在相同的基组水平上计算得到了各团簇构型的总能量和结合能,结果显示,对于团簇(C5H5N)n(H2O)4(n=1~2),团簇中的水分子形成四元环的结构要比形成三元环的结构稳定。对团簇的最高占据轨道与最低空轨道之间的能隙分析发现,团簇C5H5N(H2O)4的最低能量结构具有较高的稳定性,可能具有幻数结构;最后,分析讨论了吡啶-水团簇的红外振动光谱,对较强的谱峰进行了指认。     

纳米团簇熔化过程的分子动力学模拟

本文采用分子动力学结合嵌入原子多体势,模拟了不同半径的Ni纳米团簇的升温熔化过程,研究团簇尺寸对熔点和表面能的影响.模拟结果表明:团簇的熔点显著低于体材料的熔点.团簇熔化的过程首先是在团簇的表面出现预熔,然后向团簇内部扩展,直到整个团簇完全熔为液态.在模拟的纳米尺度范围内,团簇的熔点与团簇尺寸基本成线性关系.团簇的表面能随着团簇尺寸的增大而减小,而且表面能均高于体材料的表面能.     

超声喷流氩氢混合团簇特性研究

利用瑞利散射方法研究了超声喷流Ar-CH4混合团簇和超声喷流Ar-H2混合团簇的特性.通过测量不同混合比例和不同背压下所形成混合团簇的散射信号发现,当用Ar气和CH4的混合气体进行超声喷流时很容易形成Ar-CH4混合团簇,当Ar气含量为50%时混合团簇尺度最大且大于相同气压下纯Ar团簇尺度和纯CH4团簇尺度.实验发现,与纯H2团簇只能在低温条件下获得不同,常温下即可形成Ar-H2混合团簇,实现了常温下含氢团簇的获取,从而有效降低了制备成本.在H2含量大于40%时混合团簇开始形成并在60%时达到最大尺度.含氢(氘)混合团簇在氢(氘)团簇的基础上引入了更重的异核Ar元素,在激光氘团簇聚变实验中它将进一步加速氘离子从而获得更高的能量,并具有更高的中子产额和聚变效率.     

硅团簇熔化行为的紧束缚分子动力学研究

利用紧束缚分子动力学方法研究了硅团簇Si_n(n=5—10)的熔化行为.给出了团簇 熔化潜热 和熔点随团簇尺寸的变化关系，表明团簇熔化潜热和熔点强烈依赖于团簇的原子数.计算结 果表明硅团簇熔化机理与金属团簇熔化有很大不同，金属小团簇的熔化是一个从低温类固态 向高温类固态转变的过程，在转变温区，类固态和类液态处于动力学共存，而硅团簇在转变 温区则是处于一种中间态，这种中间态既不是类固态又不是类液态.比较了用不同计算方法 和定义方法所得硅团簇熔点. 关键词： 紧束缚 硅团簇 熔化潜热     

H3+团簇离子与固体相互作用

报道了H3+团簇通过碳膜对产生的各种产物的测量结果.分析讨论了三原子离子团簇与固体相互作用中的电荷交换过程.证明在产物的形成中,电荷交换过程起关键作用.分析研究了H3+团簇与固体作用中的团簇效应和尾流效应. 关键词： H3+团簇 电荷交换 团簇效应 尾流效应     

基于极紫外自由电子激光的中性团簇红外光谱

团簇在能源催化和大气雾霾等诸多化学过程中广泛存在,团簇表征与性能研究对诠释化学反应机理至关重要. 然而,中性团簇由于缺乏电荷、难于探测,实验研究非常困难. 鉴于上述情况,发展了基于极紫外自由电子激光的中性团簇红外光谱实验方法,用于质量选择中性团簇的高灵敏探测、结构表征和性能研究. 红外-极紫外衰减和红外+极紫外增强光谱实验方法已被应用于一些中性水团簇和一些中性金属羰基化合物的研究. 由于极紫外自由电子激光的波长范围涵盖了绝大多数中性团簇的第一电离势,这一独特的实验方法为开展各类中性团簇红外谱学和结构的研究打开了大门. 本文综述了这些红外光谱实验方法及其在中性团簇研究中的应用.     

利用密度泛函理论对MgBen(n=2-12)团簇的结构及其电子性质

利用密度泛函理论对MgBen(n=2-12)团簇的结构和电子性质进行了研究. 较高的能隙和结合能都表明，3和9是团簇的幻数；随着团簇尺寸的增加，Be原子间的相互作用由范德瓦尔斯到共价键以及金属键过渡. 与Be主团簇相比，MgBen(n=2-12)团簇较早地出现了金属性. 通过电子性质的分析发现，掺杂Mg原子降低了主团簇的稳定性.     

密度泛函理论研究Scn,Yn和Lan(n=2—10)团簇的稳定性、电子性质和磁性

通过采用密度泛函理论对Sc2,Y2和La2基本性质的计算,选择在较优理论水平下系统地研究了Scn,Yn和Lan(n=2-10)团簇的几何结构、稳定性、电子性质和磁性及其随团簇尺寸的变化趋势.此同族三种团簇的稳定性由原子密堆集几何结构效应决定,幻数均表现出一致的结果.Lan团簇的能隙比Scn和Yn团簇的能隙大,计算获得了团簇的电离势和电子亲和势数据,Yn团簇的电离势与实验值相符,最小极化率规律可很好地表征团簇的稳定性.三种团簇均具有较大的磁矩,磁矩与团簇的自旋多重度、几何和电子结构密切相关,理论值与实验值符合较好,随着团簇尺寸的增加三种团簇的平均磁矩总体上都呈递减的趋势并有局部振荡的特征.     

Pd_nAl~(±)(n=1—8)二元团簇的密度泛函理论研究

采用密度泛函理论(DFT)方法,在BPW91/LANL2DZ水平下详细研究了PdnAl±(n=1—8)团簇的几何结构、稳定性和电极化率,并与Pdn+1和PdnAl(n=1—8)团簇进行了比较.结果表明:除n=6,8外,PdnAl团簇和Pdn+1团簇的基态结构保持了相同的构型,除Pd2Al±和Pd6Al+外,PdnAl±团簇的基态结构与PdnAl团簇的保持了相同的结构.且在PdnAl和PdnAl±团簇基态结构中,Al原子位于较高的配位点上.分裂能和二阶能量差分的分析结果表明Pd4,Pd3Al和Pd3Al±团簇相对其他团簇具有较高的稳定性.极化率的研究表明富Pd团簇的非线性光学效应强,容易被外场极化.Pd6,Pd5Al和Pd3Al±团簇的极化率各向异性不变量为最小值,说明相应团簇对外场的各向异性响应最弱,各方向的极化率大小变化不大.     

Raman investigations of TiO2 nanotube substrates covered with thin Ag or Cu deposits

A tubular array of TiO₂ nanotubes on Ti matrix was used as a support for Ag or Cu sputter‐deposited layers intended for surface‐enhanced Raman scattering (SERS) investigations. The composite samples of Ag/TiO₂–nanotube/Ti and Cu/TiO₂–nanotube/Ti were studied with the aid of scanning electron microscopy (SEM) and Auger electron spectroscopy (AES) [and scanning Auger microscopy (SAM)] to reveal their characteristic morphological and chemical features. Raman spectra of pyridine (as a probe molecule) were measured after it had been adsorbed on the TiO₂–nanotube/Ti substrates covered with thin Ag or Cu deposit as well as on the bulk electrochemically roughened Ag or Cu reference substrates. It was found that the SERS spectra measured for pyridine adsorbed on the bulk silver substrate were significantly different than the spectra measured on the TiO₂–nanotube/Ti substrates covered the Ag layer. The spectra measured for pyridine adsorbed on the Ag/TiO₂–nanotube/Ti suggest that on the surface of such a composite substrate there are many Lewis acidic sites. Spectra typical for pyridine adsorbed on acidic sites were observed even after deposition of a relatively thick silver layer (e.g. an Ag layer with an average thickness of 80 nm) on the TiO₂–nanotube/Ti support. Our findings suggest that TiO₂–nanotube/Ti support is a promising substrate for the preparation of metallic nano‐clusters on a support containing acidic active sites. Copyright © 2009 John Wiley & Sons, Ltd.     

Plasma resonance — enhanced raman scattering by absorbates on gold colloids: The effects of aggregation

The excitation profile of the 1014 cm^?1 Raman band of pyridine adsorbed on colloidal gold particles, and the extinction and elastic scattering spectra of the colloids, are measured as the colloids slowly aggregate in the presence of pyridine. Transmission electron microscopy shows that the aggregates formed are predominantly strings of particles rather than compact clusters, and the dipolar plasma modes of the aggregates are therefore split into longitudinal and transverse components. It is shown that only for excitation under the longitudinal resonance extinction band is there a large Raman intensity enhancement. The Raman excitation profile maximum corresponding to excitation under this resonance moves progressively to longer wavelengths, increasing substantially in height, as the aggregation proceeds. Thus aggregation is most advantageous for the realization of large Raman signals from these colloids, the Raman intensity at a given excitation wavelength increasing approximately as the square of the absorbance at that wavelength as the aggregation proceeds. These observations are discussed in relation to the electromagnetic field enhancement contribution to the surface Raman effect, with which they are in general agreement, and the large increase in ¦?¦² for gold and silver with increase in wavelength is shown to be a significant factor in accounting for some of these effects of aggregation.     

Surface-enhanced Raman scattering (SERS) activity of Ag, Au and Cu nanoclusters on TiO2-nanotubes/Ti substrate

Tubular arrays of TiO₂ nanotubes (ranging in diameter from 40 to 110 nm) on a Ti substrate were used as a support for Ag, Au or Cu deposits obtained by the sputter deposition technique, where the amount of metal varied from 0.01 to 0.2 mg/cm². Those composite supports were intended for surface-enhanced Raman scattering (SERS) investigations. Composite samples were studied with the aid of scanning electron microscopy (SEM) and Auger electron spectroscopy (AES) to reveal their characteristic morphological and chemical features. Raman spectra of pyridine (as a probe molecule) were measured at different cathodic potentials ranging from −0.2 down to −1.2 V after the pyridine had been adsorbed on the metal-covered TiO₂ nanotube/Ti substrates. In addition, SERS spectra on a bulk standard activated Ag, Au and Cu substrates were also measured. The SERS activity of the composite samples was strongly dependent on the amount of metal deposit, e.g. at and above 0.06 mg Ag/cm², the intensity of SERS signal was even higher than that for the Ag reference substrate. The high activity of these composites is mainly a result of their specific morphology. The high SERS sensitivity on the surface morphology of the substrate made it possible to monitor very small temporal changes in the Ag metal clusters. This rearrangement was not detectable with microscopic (SEM) or microanalytical (AES) methods. The SERS activity of Au or Cu clusters was distinctly lower than those of Ag. The spectral differences exhibited by the three kinds of composites as compared to the reference metal samples are discussed.     

The effect of an anti-hydrogen bond on Fermi resonance:A Raman spectroscopic study of the Fermi doublet ν1-ν12 of liquid pyridine

The effects of an anti-hydrogen bond on the ν1-ν12 Fermi resonance(FR) of pyridine are experimentally investigated by using Raman scattering spectroscopy.Three systems,pyridine/water,pyridine/formamide,and pyridine/carbon tetrachloride,provide varying degrees of strength for the diluent-pyridine anti-hydrogen bond complex.Water forms a stronger anti-hydrogen bond with pyridine than with formamide,and in the case of adding non-polar solvent carbon tetrachloride,which is neither a hydrogen bond donor nor an acceptor and incapable of forming a hydrogen bond with pyridine,the intermolecular distance of pyridine will increase and the interaction of pyridine molecules will reduce.The dilution studies are performed on the three systems.Comparing with the values of the Fermi coupling coefficient W of the ring breathing mode ν1 and triangle mode ν12 of pyridine at different volume concentrations,which are calculated according to the Bertran equations,in three systems,we find that the solution with the strongest anti-hydrogen bond,water,shows the fastest change in the ν1-ν12 Fermi coupling coefficient W with the volume concentration varying,followed by the formamide and carbon tetrachloride solutions.These results suggest that the stronger anti-hydrogen bond-forming effect will cause a greater reduction in the strength of the ν1-ν12 FR of pyridine.According to the mechanism of the formation of an anti-hydrogen bond in the complexes and the FR theory,a qualitative explanation for the anti-hydrogen bond effect in reducing the strength of the ν1-ν12 FR of pyridine is given.     

Direct visual evidence for the chemical mechanism of surface‐enhanced resonance Raman scattering via charge transfer

We describe the chemical and electromagnetic enhancements of surface‐enhanced resonance Raman scattering (SERRS) for the pyridine molecule absorbed on silver clusters, in which different incident wavelength regions are dominated by different enhancement mechanisms. Through visualization we theoretically investigate the charge transfer (CT) between the molecule and the metal cluster, and the charge redistribution (CR) within the metal on the electronic intracluster collective oscillation excitation (EICOE). The CT between the metal and the molecule in the molecule–metal complex is considered as an evidence for chemical enhancement to SERRS. CR within the metal on EICOE is considered as an evidence for the electromagnetic enhancement by collective plasmons. For the incident wavelength from 300 to 1000 nm, the visualized method of charge difference density can classify the different wavelength regions for chemical and electromagnetic enhancement, which are consistent with the formal fragmented experimental studies. Copyright © 2008 John Wiley & Sons, Ltd.     

氯铝酸离子液体酸性的红外光谱探针和量子化学研究

文章采用吡啶探针红外光谱、吡啶递增吸附实验研究和量子化学理论计算相结合的方法深入研究了氯铝酸离子液体的酸性及氯铝酸离子液体Lewis酸位Al₂Cl-₇与吡啶吸附之间的相互作用机理。通过实验和理论计算研究发现,Al₂Cl-₇,AlCl-₄阴离子具有吸电性,能够吸引吡啶环上的孤对电子产生吸附作用,具有Lewis酸性,它们分别呈现吡啶探针红外光谱Lewis酸特征峰;通过红外光谱特征峰峰位、键长及电荷分布分析表明Al₂Cl-₇的酸性强于AlCl-₄;氯铝酸离子液体Lewis酸位Al₂Cl-₇与吡啶吸附的机理为：当吡啶含量小时,仅存在Py-Al₂Cl-₇吸附;当吡啶量增加到一定程度时,Py-Al₂Cl-₇配位络合物中的AlCl-₄容易与吡啶发生吸附解离为Py-AlCl-₄配位络合物和Py-AlCl₃配位络合物,导致离子液体吡啶递增吸附红外特征峰发生变化。     

Quantification of the Number of Silanol Groups in Silicalite and Mesoporous MCM-41: Use of Ft-Raman Spectroscopy

Infrared and FT-Raman spectra have been obtained on pyridine adsorbed within two siliceous materials, silicalite and MCM-41. Both spectroscopic techniques detect the presence of weak physisorbed pyridine and stronger hydrogen-bonded pyridine. In particular, the FT-Raman spectra are well resolved and can be used to measure the number of pyridine molecules that interact with hydroxyl groups. for silicalite, it is found that an average of one pyridine molecule per unit cell interacts with hydroxyl groups. the number of hydroxyl groups present at the surface of porous silica materials can also be obtained using this approach. for siliceous MCM-41, it is found that the hydroxyl group concentration is about 3 mmol/g of dry solid.     

The detection by SERS of resonantly excited desorption of pyridine from silver island films by IR laser absorption

We have shown that when a very thin film of pyridine about two or three monolayers thick on a silver island film is exposed to a pulsed CO₂ laser line whose frequency corresponds to that of a pyridine vibrational mode the physisorbed molecules within the pyridine film can be desorbed even at liquid He temperatures. It is interesting that this observation was first made using surface enhanced Raman scattering. Experimental results are presented from which it is concluded that the phenomenon can be described as resonantly excited desorption. The absorbed IR energy seems to be localized within the pyridine film and the silver film and thermallized to some degree causing some of the physisorbed molecules to desorb. Analysis of the SERS spectra before and after the resonantly excited desorption has enabled us to separate out the SERS spectra due to the physisorbed pyridine and the chemisorbed pyridine.     

利用吡啶添加剂提高钙钛矿太阳能电池的光伏性能

研究了吡啶作为添加剂对一步法制备甲胺铅碘钙钛矿太阳能电池光电性能的影响.利用SEM、AFM、XRD、UV-Vis、PL等手段研究了不同吡啶掺杂浓度对制备的CH3 NH3 PbI3薄膜的表面形貌、结晶度和光学性能的影响.研究结果表明:少量的吡啶掺杂可以提高钙钛矿薄膜的覆盖率及降低薄膜的表面粗糙度.当在CH3 NH3 PbI3前驱体溶液中添加体积分数为1%的吡啶时,制备的钙钛矿太阳能电池的能量转换效率达到7.33%,而未加吡啶的对比器件效率仅为1.01%.进一步添加吡啶会导致钙钛矿材料的降解.     

Identification of species formed after pyridine adsorption on iron,cobalt, nickel and silver electrodes by SERS and theoretical calculations

The adsorption of pyridine (py) on Fe, Co, Ni and Ag electrodes was studied using surface‐enhanced Raman scattering (SERS) to gain insight into the nature of the adsorbed species. The wavenumber values and relative intensities of the SERS bands were compared to the normal Raman spectrum of the chemically prepared transition metal complexes. Raman spectra of model clusters M₄(py) (four metal atoms bonded to one py moiety) and M₄(α‐pyridil) where M = Ag, Fe, Co or Ni were calculated by density functional theory (DFT) and used to interpret the experimental SERS results. The similarity of the calculated M₄(py) spectra with the experimental SERS spectra confirm the molecular adsorption of py on the surface of the metallic electrodes. All these results exclude the formation of adsorbed α‐pyridil species, as suggested previously. Copyright © 2009 John Wiley & Sons, Ltd.