以(真空紫外光+紫外光)-共振加强式多光子游离法侦测交叉分子束之甲基生成物

用(真空紫外光+紫外光)-共振加强式多光子游离法侦测甲基自由基.为证明此法之灵敏度,实验用交叉分子束反应F+CH4(CD4)→HF(DF)+CH3(CD3),其绝对灵敏度可达107/cm3.由所得之光谱,更精确地得到两个里德堡态3d2E″及3d 2A1′之光谱系数.     

乙烯自由基A2A''(v'=0)←X2A'(v''=0)带的转动分析

通过193 nm光解丁烯酮分子产生乙烯基自由基(C₂H₃). 经射流冷却后, 用另一束激光光解C₂H₃, 生成的氢原子碎片经共振增强多光子电离(REMPI)过程, 记录氢离子信号随光解波长变化, 得到20020～20070 cm_-1范围内乙烯基激发的转动分辨光谱. 该谱对应于A²A'(v'=0)←X²A'(v'=0)跃迁的转动结构. 结合量子化学理论计算、光谱拟合以及前人的研究结果, 对该段光谱进行了完整的转动识别, 确定了40条转动谱线的位置. 由光谱拟合还得到A²A'(v'= 0 )能级的预解离寿命为3.3 ps, 且不依赖于转动量子数.     

离子速度成像方法研究C8H17Br分子的光解动力学

用离子速度成像方法, 研究了长链C8H17Br分子在234 nm激光下的光解过程. 通过2+1共振增强多光子电离探测了两种光解产物Br*(2P1/2)和Br(2P3/2), 得到了它们的相对量子产率. 从光解产物Br*(2P1/2)和Br(2P3/2)的速度图像得到了能量和角度分布. 并根据相对量子产率和角度分布, 计算了不同解离通道的比例. 实验发现C8H17Br分子解离过程中大部分能量都转化为内能, 该能量分配可以较好地用软反冲模型来解释, 并分析了这种能量分配跟烷基大小的关系.     

Experimental and Theoretical Investigation of the 3sp(d) Rydberg States of Fenchone by Polarized Laser Resonance-Enhanced-Multiphoton-Ionization and Fourier Transform VUV Absorption Spectroscopy

The VUV absorption spectrum of fenchone is re-examined using synchrotron radiation Fourier transform spectrometry, revealing new vibrational structure. Picosecond laser (2+1) resonance enhanced multiphoton ionization (REMPI) spectroscopy complements this, providing an alternative view of the 3spd Rydberg excitation region. These spectra display broadly similar appearance, with minor differences that are largely explained by referring to calculated one- and two-photon electronic excitation cross-sections. Both show good agreement with Franck-Condon simulations of the relevant vibrational structures. Parent ion REMPI ionization yields with both femtosecond and picosecond excitation laser pulses are studied as a function of laser polarization and intensity, the latter providing insight into the relative two-photon excitation and one-photon ionization rates. The experimental circular-linear dichroism observed in the parent ion yields varies strongly between the 3s and 3p Rydberg states, in good overall agreement with the calculated two-photon excitation circular-linear dichroism, while corroborating other evidence that the 3p_z sub-state plays no more than a very minor role in the (2+1) REMPI spectrum. Vibrationally resolved photoelectron spectra are recorded with picosecond pulse duration (2+1) REMPI at selected intermediate vibrational excitations. The 3s intermediate state displays a very strong Δv=0 propensity on ionization, but the 3p intermediate evidences more complex vibronic dynamics, and we infer some 3p→3s internal conversion prior to ionization.     

Vibrational Spectrum of o‐Dimethoxybenzene in the S1 and D0 States

The optimized molecular geometries of o‐dimethoxybenzene (ODMB) in the S₀ state were predicted by ab initio and density functional theory calculations. Its vibrational spectra in the S₁ and D₀ states were studied by one color resonant two photon ionization (1C‐R2PI) and mass analyzed threshold ionization (MATI) experiments. The results indicated that trans rotamer was most stable. Only one rotamer of ODMB was detected by the 1C‐R2PI spectra, and its band origin was (35750±2) cm^?1, its ionization energy was (61617±5) cm^?1. Most of the observed vibrations in the D₀ state resulted from the in‐plane ring and substituent sensitive modes.     

S(1D)+D2反应的立体动力学理论研究

在abinitio势能面上利用非含时量子反应散射理论研究了S(1D) D2反应在散射能为22.18kJ·mol-1时的立体动力学.计算的微分反应截面呈现弱反对称的前向后向散射,这一结果与以前的准经典结果和实验结果相一致.态分辨的极化依赖的微分反应截面和极化参数显示产物极化并非各向异性分布,这意味着在反应过程中由于势能面上存在一个深势阱从而形成了长寿命的复合物.     

Halogen Effect on the Photodissociation Mechanism for Gas‐Phase Bromobenzene and Iodobenzene

The velocity imaging technique combined with (2+1) resonance‐enhanced multiphoton ionization (REMPI) is used to detect the halogen fragments in the photodissociation of bromobenzene and iodobenzene at 266 nm. With the aid of potential energy curve calculations by Lunell (Y. J. Liu, P. Persson, S. Lunell, J. Phys. Chem. A 2004 , 108, 2339–2345.), the Br fragmentation is proposed to stem from excitation of the lowest excited singlet state followed by predissociation along a repulsive triplet state. The slowed dissociation rate leads to production of the isotropic Br fragments and 93 % internal energy deposition. Only the ground state Br(²P_3/2) is detectable. In contrast, when iodine is substituted, the iodine effect stabilizes the repulsive states associated with the I? C₆H₅ bond rupture and the subsequent dissociation channels become more complicated. 84 % of the iodobenzene molecules obtained follow a direct dissociation channel, while the remaining undergo a predissociative process. Both routes result in rapid dissociation with anisotropy parameters of 0.7±0.2 and 0.9±0.2 as well as 70 % and 26 % in the fractions of translational energy deposition, respectively. The relative quantum yields of I* and I are 0.35 and 0.65 and their related photodissociation pathways are discussed in detail.     

分子整流的实验与理论研究进展*

分子电子器件的思想始于20世纪70年代,分子整流的研究在30多年中取得了显著进展,包括分子结构设计、实验测量以及理论模拟。本文简述了分子整流的发展历程,介绍了被广泛研究的分子整流体系以及分子水平整流机理,包括D-σ-A型、D-π-A型、D-A型、构象转变和界面引起的整流,以及负微分电阻现象。最后提出了分子整流研究中存在的一些问题,并展望了分子整流的研究和发展方向。     

(1+1) Resonance‐Enhanced Multiphoton Ionization and Photodissociation Study of CS2 via the 1B2 State

(1+1) resonance‐enhanced multiphoton ionization (REMPI) spectra of CS₂ and molecular dissociation dynamics are investigated using a time‐of‐flight mass spectrometer equipped with velocity imaging detection. The REMPI spectra via a linear‐bent →¹B₂( ) transition are acquired in the wavelength range of 208–217 nm. Each ro‐vibrational band profile of the ¹B₂( ) state is deconvoluted to yield the corresponding predissociative lifetime from 0.3 to 3 ps. Upon excitation at 210.25 and 212.54 nm, the resulting images of S⁺ and CS⁺ fragments are analyzed to give individual translational energy distributions, which are resolved into two components corresponding to the CS+S(³P) and CS+S(¹D) channels. The product branching ratios of S(³P)/S(¹D) are evaluated to be 5.7±1.0 and 9.6±2.5 at 210.25 and 212.54 nm, respectively. Despite the difficulty avoiding the effect of multiphoton absorption, the molecular dissociation channel is verified to prevail over the dissociative ionization channel of CS₂. The anisotropy parameters for the triplet and singlet channels are determined to be ～0.8 and 1.1–1.3, respectively, suggesting that the predissociative state should have a bent configuration with a short lifetime.     

Multiphoton dissociation of some aromatic molecules. Formation of atomic carbon in the 2p21S0 excited state

Carbon atoms in the high energy metastable state 2p^{2 1}S⁰ have been detected for the first time in multiphoton dissociation of some aromatic molecules, using tunable laser light in the region of 380 to 393 nm. The detection is based on the two-photon resonances2p ¹S₀ → → 3p¹D₂ and 2p¹S₀ → → 3p¹S₀ three-photon ionization of atomic carbon, following the dissociation of the molecule, during the same laser pulse. The results are of particular interest in the field of nonlinear photochemistry.     

Theoretical Study of Electron Density Delocalization in the Excited States of Transition Metal Complexes

This paper presents a theoretical study of electron density delocalization effects over an electron-accepting ligand in metal-to-ligand charge-transfer (MLCT) complexes in the excited states, where the ligand is 4,4'-X₂-2,2'-bpy (X = H, NH₂, CH₃, Ph, Cl, CO₂Et, NO₂, bpy = 2,2'-bipyridine) or terpy (2,2':6',2'-terpyridine). Optimal geometry calculations are performed for neutral ligand molecules and their radical anions modeling the state of the ligands during MLCT excitations. Spin density distribution over atoms in the radical anions is used as a measure of the degree of delocalization. The role of spin density distribution in excitation-induced changes of geometrical parameters of the ligands is considered.     

金镍二元团簇结构和电子性质的理论研究

在UBP86/LANL2DZ和UBP86/def2-TZVP水平下详细研究了AumNin (m＋n≤6)团簇的几何结构和电子性质. 详细地分析了团簇的结构特征, 平均结合能, 垂直电离势, 垂直电子亲和能, 电荷转移以及成键特征. 所有混合团簇中, 镍原子趋于聚集到一起, 形成最多Ni—Ni键, 金原子分布在镍原子聚集体周围以形成最多Au—Ni键. Ni原子较少团簇的电子性质与纯金团簇类似, 呈现一定奇偶振荡. 混合团簇中存在镍到金原子间的电荷转移. Ni原子较少团簇中, 自旋电子主要定域在Ni原子上, Ni原子较多团簇中, Au原子明显受到自旋极化. 混合团簇的分波态密度表明, AuNi混合团簇对小分子的反应活性要高于纯金团簇.     

Vibronic spectral behavior of molecules. XIII. Theoretical contribution to the vibronic coupling and the dushinsky effect on the S1 ← S0 absorption and the S1 → S0, S2 → S1, and S2 → S0 fluorescences of azulene

Based on the completely optimized S₀, S₁, and S₂ molecular geometries of azulene, the vibronic structure of the S₁ ← S₀ absorption as well as of the S₁ → S₀, S₂ → S₁, and S₂ → S₀ fluorescences is investigated theoretically within the adiabatic approximation. By means of theory-experiment comparisons, the influence of non-Condon terms and of the Dushinsky effect on the vibronic structure of azulene spectral behavior is discussed. Typical for the S₁ ← S₀ absorption and the S₁ → S₀ fluorescence are vibronic transition moment contributions of Condon type, whereas the interpretation of azulene S₂ → S₁ and S₂ → S₀ fluorescences is successful only within the scope of the Herzberg–Teller approach by taking into account vibronic coupling terms and, additionally, the Dushinsky effect in the latter case. An analysis of the relevant vibrational modes is given.     

Experimental and Theoretical Study of the Impact of Alumina Droplets on Cold and Hot Substrates

A complex experimental set-up was built to study the impact of liquid alumina droplets on different substrates (stainless steel 304L, sintered alumina, carbon–carbon) kept at temperatures up to 2100 K. The impact behavior: rebound, deposition, splashing, spattering was systematically studied as well as the resulting splat shapes. The set-up consists in a controlled atmosphere chamber where molten alumina particles with diameters between 10 and 90 m, are produced by a d.c. plasma torch, substrates being heated by a second d.c. plasma torch. In such conditions, it was possible to achieve particle temperatures between 2300 and 4200 K with velocities in the range 50 to 300 m/s. The particle behavior at impact was characterized by the Sommerfeld parameter K (K=We^1/2 Re^1/4 We and Re being respectively the Weber and Reynolds numbers of impacting particles). It was possible to vary K between 3 and 1300. Low K values were obtained by tilting the substrate up to 60°. The parameters of a single particle at impact were measured: its velocity v_p and diameter d_p by Phase Doppler Anemometry (v_p=5%, d_p=10%) and its temperature T_p by fast (100 ns) two color pyrometry (T_p=15%). The particle impact was visualized by a fast camera coupled to a microscope (exposure delay time 50 ns . . .100 ms) with complex synchronization and light intensity problems. To solve the latter, the impacting particle had to be illuminated with a 2 W c.w. Ar⁺ laser at 488 nm. Unfortunately, the controlled atmosphere chamber did not allow to change the substrate after each particle impact. Starting from a smooth surface for the first impact, due to the successively deposited splats, rapidly droplets impacted on a rough surface (Ra5 m). For splats collected on a hot alumina substrate (2100 K), where flattening is completed before solidification starts (case similar to that of ethanol droplets on cold copper) deposition occurs for K between 4 and 90 while splashing occurs for K as low as 30. These results are slightly different from those related to the ethanol droplet for which deposition occurs for 357.7. This could be due to the precision of measured values and the rough surface. For splats collected in spraying conditions splashing is always the rule K values up to 1400) especially on rough surfaces. However the particle impact velocity and temperature, the substrate temperature and tilting plays an important role on the resulting splat diameters, distortion and elongation rates. The question which is still pending is which quantity of splashed material is incorporated within the constructing coating and how does it affect its thermophysical properties.     

A Theoretical Investigation of the Decomposition Reactions of Ethyl Formate in the S1 and T1 States

This study investigates the decomposition reactions of ethyl formate in the S₁ and T₁ states. The dissociation channels leading to HCOOH + C₂H₄, CH₃CH₂O + HCO, CH₃CH₂OCO + H, and CH₃CH₂ + HCO₂ were studied. The major reactions of ethyl formate in the S₁ and T₁ states are isomerization to the biradical CH₂CH₂OC(OH)H and dissociation to CH₃CH₂O + HCO. All the stationary and intersection points were optimized at the CAS(10,8) level of theory with the 6‐31G(d,p) and 6‐311G(2df,2pd) basis sets. Single‐point CASPT3 energy was calculated for each of the stationary and intersection points. Microcanonical rate constants were also calculated for each of the reactions by using the RRKM theory.     

Proton/Hydrogen‐Transfer Coordinate of 2,5‐Dihydroxybenzoic Acid Investigated in a Supersonic Beam: Combined IR/UV Spectroscopy in the S0, S1, and D0 States

As a model system for intramolecular proton/hydrogen‐transfer coordinates, the structure of 2,5‐dihydroxybenzoic acid is investigated for the ground, first electronically excited and also the ionic state. Combined IR/UV spectroscopy in molecular‐beam experiments is applied and the experimental results are interpreted by the application of DFT and CASPT2 methods. No proton or hydrogen transfer is observed, but evidence is given for a hydrogen dislocation of the intramolecular hydrogen bond in the S₁ state and to lesser extent in the D₀ state. To obtain direct information on the proton/hydrogen‐transfer coordinate, IR spectra are recorded both in the region of the OH and especially the CO stretching vibrations by also applying two new variants of combined IR/UV spectroscopy for the S₁ and D₀ states. The CO groups are directly involved in the hydrogen bond and, in contrast to the hydrogen‐bonded OH groups, the CO stretching frequencies can be observed in all electronic states.     

Theoretical and Experimental Study of Pb2+ and Hg2+ Adsorption on Biopolymers, 1. Theoretical Study

Chitosan and pectic acid have been modeled as disaccharides or oligosaccharides for Hg²⁺ and Pb²⁺ adsorption. Reasonable models of both biopolymers were used. Several adsorption sites of both polysaccharides were considered, mainly NH₂ in chitosan and CO₂^– in pectic acid. Hg²⁺ has several points of anchorage on chitosan. The most important one is NH₂ . The Molecular Mechanic modeling permit us to compare in relative terms the different conformations of models of pectic acid and chitosan and their effect in heavy metal coordination. Using the Parameterized Model version 3 (PM3), we report the formation enthalpy of inter‐ and intramolecular compounds with Hg and Pb. The Extended Huckel method (EHM) results seem to indicate that electrostatic interaction (leading to adsorbed cation on NH₂ and on sites different to NH₂) could be the reason for the high uptake found for Hg²⁺ using chitosan. Besides NH₂, the OH near the amine group is the preferred site for Hg²⁺ adsorption, especially if it is ionized. In the case of Pb²⁺ adsorption, several sites of chitosan present no interaction with this cation. Only the NH₂ group and the ionized OH group mentioned above seem to be the preferred sites, following the EH modified (EHMO) results. The Hg‐ and Pb‐adsorption modeling on pectic acid permit us to conclude that the best site is the same for both metals: the bridge oxygen between monomers of galacturonic acid. the carbonyl group from carboxylate is the best second site for Hg²⁺, whereas the internal oxygen bridge is the best second site for Pb²⁺. Considering the Hg ²⁺ chemistry in aqueous solution, we evaluated the HgOH⁺ and HgCl⁺ or HgCl₃^– adsorption on both copolymers, using EHMO. The energetic of adsorption changed on both biopolymers for these species, comparing them with Hg²⁺.     

化学反应散射共振态的实验检测与理论模拟

化学反应中的散射共振态（或称反应性共振）控制着化学反应的分支比、产物的态分布及空间分布等。反应性共振的实验检测分为间接法和直接法。从理论上,一是构造反应体系的势能面,从势能面过渡态的结构来研究散射共振态;二是计算态-态反应动力学,尤其是用寿命矩阵来研究散射共振态。本文介绍反应性散射共振态的实验检测及理论模拟方法,并对今后的发展动向作出展望。     

The Formation of the Cluster Ions NH_5~ and (NH_3)_2H_2~ and ab initio Calculation Study of Their Structures

AmmoniaclusterhasbeenwidelystUdiedbymanygroups'~'.The'mainionsmeasuredinthemassspectraareprotonatedammoniaclusterions,whichareproducedfromtheion-moleculereactionsintheionizedammoniaclusters.ShinoharaandNishi4'5foundtheionswhosemasswereIamu.largerthantheprotonatedammoniaclusterionsbythemethodofMPIMS.Theyattributedtheseionstothebinaryclusterions[(NH,)nNH. 1H,Ocomingfromwaterastheimpurityintheammoniasample.BugaetsandZhogolev'predictedtheoreticallytheprobabilityoftheexistenceofthehypervalenc…     

Theoretical and Experimental Investigation of the Production of PMMA-Based Bone Cement

Poly(methyl methacrylate) (PMMA)-based polymers have been extensively used for manufacturing of artificial bone cements for treatment of osteoporosis. A typical bone cement recipe contains methyl methacrylate, which polymerizes in situ during cement application. An inherent problem of this reaction is the high amount of heat released during the cement preparation, which may lead to irreparable damage of living tissues. Optimization of PMMA-based bone cement (PMMABC) recipes is thus an important step towards safe and reliable clinical usage of these materials. A theoretical and experimental investigation is performed here to unveil the influence of some preparation variables on the production of PMMABC and to allow for future optimization of the PMMABC recipe. It is shown that the degree of mixing of the components of the recipe plays a fundamental role on the development of the temperature profile. For this reason, the PMMABC obtained with the in-situ blending of PMMA and barium sulfate during the suspension polymerization leads to much better homogeneity of the final test pieces and improved control of the temperature profile.