氟原子与溴代甲烷反应化学发光研究

用光子计数技术系统地探测了F(^2P)原子与溴代甲烷等(CH~3Br、CH~2Br~2和CHBr~3)反应在各种压力下的可见区(300～900nm)化学发光,得到HF电子基态振动泛频跃迁及 Br~2(B)、BrF(B)、CHF(A)、CH(A) 等分子电子激发态跃迁的发射谱.求出HF(υ=3)转动温度为480K,计算机模拟光谱获得了Br~2(B)的振动布居.对比F与氯代甲烷反应的机理分析表明,初级反应主要是F提取形成HF,多级反应产生了电子激发态的产物分子.     

氟原子与乙腈、丙腈反应化学发光研究

我们研究了CF~4/Ar混合气体微波放电产生的基态F(^2P)原子与CH~3CN,CH~3CH~2CN发生的反应,观测了不同压力下两个反应的可见区(400～900nm)化学发光.获得了产物碎片HF≠(X),CN^*(A),CH^*9(A,B)的发射光谱.并计算了CN(A→X)跃迁的Franck-condon因子以及CN(A) 态的振动布居.机理分析认为CN^*(A)是由次级反应产生的激发态分子(如CH~2CNF^*)离解而形成.     

F与自由基CH~2OH反应理论研究

用量子化学从头计算法对氟原子与羟亚甲基CH~2OH在势能面上的反应进行了研究。采用G2(MP2,SVP)理论计算出了热能面上各驻点物种的构型参数、振动频率和能量。结果表明:F与CH~2OH反应首先通过H转移形成甲基,然后甲基旋转,再通过甲基中一个H与F结合,最后产生HF和CH~2O。计算出反应热为455.9kJ.mol^-^1,与实验值439kJ.mol^-^1符合较好。另外对前人红外吸收光谱研究中没有观测到CHOH提出了可能解释。     

氟原子与溴代甲烷反应化学发光研究

用光子计数技术系统地探测了F(~2P)原子与溴代甲烷等(CH_3Br、CH_2Br_2和GHBr_3)反应在各种压力下的可见区(300～900 nm)化学发光,得到HF电子基态振动泛频跃迁及Br_2(B)、BrF(B)、GHF(A)、CH(A)等分子电子激发态跃迁的发射谱.求出HF(v=3)转动温度为480 K,计算机模拟光谱获得了Br_2(B)的振动布居.对比F与氯代甲烷反应的机理分析表明,初级反应主要是F提取H形成HF,多级反应产生了电子激发态的产物分子。     

F~2+2HCl→2HF+Cl~2反应机理的密度泛函理论研究

用密度泛函理论(DFT)B3LYP方法,在6-311G^*^*基组下,计算研究了反应F~2+2HCl→2HF+Cl~2的机理。求得各可能反应途径的系列过渡态,并通过振动分析和内禀反应坐标(IRC)分析加以证实。比较反应能垒(理论计算活化能)发现,标题反应若以分子与分子作用机理进行,则需克服的最大能垒为150.63kJ.mol^-^1;若以F~2分子先裂解为F原子再反应的机理进行,则需越过能垒154.82kJ.mol^-^1,求得反应F+HCl→HF+Cl的线形和三角形两种过渡态,以三角形较稳定;求得反应HCl+Cl→H+Cl~2的两种过渡态,以线形较稳定。     

CHF2CH3(HFC-152a)与F反应的反应途径及反应速率常数研究

本文用从头计算法(UMP2/6-31G)对氟与二氟乙烷的与1位、2位碳相连的氢的抽提氢反应进行研究。CHF2CH3+F→CF2CH3+HF(R1), CHF2CH3+F→CHF2CH2+HF(R2)。在内禀反应坐标(IRC)的势能剖面基础上用传统过渡态、变分过渡态理论计算了上述两个反应的速率常数及比值, 获得了与实验相一致的结果。     

脂肪胺分子离子及质子化脂肪胺分子的碎裂反应

应用碰撞诱导解离(CID)技术研究了电子轰击方法产生的脂肪胺分子离子和化学电离方法产生的质子化脂肪胺分子的碎裂反应。质子化脂肪胺碰撞活化后的主要碎裂通道包括丢失C~XH~2~X、C~XH~2~X~+~1、C~XH~2~X~+~2单元及NH~3和生成[C~yH~2~y~+~1]^+及CH~3CH=NH~2^+离子。脂肪胺分子离子碰撞活化后的主要碎裂通道是丢失C~XH~2~X、C~XH~2~X~+~1及NH~3和生成[C~mH~2~m~-~1]^+、CH~2NH~2^+及CH~3CHNH~2^+离子。随着碰撞能的增加，远电荷碎裂反应和电荷诱导碎裂反应之间竞争引起产物离子的分布发生变化，如[C~mH~2~m~-~1]^+和[C~yH~2~y~+~1]^+离子。自由基机理可以解释质子化脂肪胺分子的远电荷反应。分子内氢抽取可以解释脂肪胺分子离子的碎裂反应。     

分子束技术研究Ba与CHCl~3, CCl~4的反应

本文分别在交叉分子束和分子束-气体条件下, 利用化学发光方法, 研究了Ba(^3D)+CH~2Cl~2, CHCl~3,CCl~4和Ca(^1S~O),Ca(^3P),Ba(^1S～O)Ba(^3D)+CCl~4的反应, 实验得出了Ba(^3D)与CH~2Cl~2, CHCL~3, CCl~4反应时, A^2II,B~2Σ^+态BACl产物的发光截面对反应物碰撞能的依赖关系和反应阈能, 以及Ba(^3D)与CCl~4反应时, 产生电子激发态BaCl产物的光子产率。发现当Ba,Ca被激发到亚稳态时, Ba+CCl~4的反应电子基态BaCl产物的振动激发增加; 而Ca+CCl~4的反应电子基态CaCl产物的转动激发增加. 并针对以上结果进行分析讨论。     

F（2P）与CH2Br2反应的化学发光光谱及其动力学

氟原子与卤代甲烷反应的化学发光研究有助于发现新的化学激光介质。氟原子与含氢卤代甲烷的反应存在F夺H的初级反应.Braynis等研究了高气压(60 Pa)下F与CH_nI_(4-n)(n=0,1,2,3)的反应,也研究了F与CH_3Br反应的化学发光,观察到了HF~?(X),CHF~*(A),CH~*(A)以BrF~*(B)的发射谱,对这些产物形成机制进行了解析并推断有中间络合物的生成.本文首次研究了F与CH_2Br_2的化学发光,在可见光范围(400～900nm)内观察了单次及多次碰撞条件下的光谱,证明在单次碰撞条件下(气压小于10~(-2)Pa)存在氟夺氢而生成HF~≠(X,V≤3)通道.而在多次碰撞条件下(气压大于0.1Pa)则观察到Br~*_2(B)和BrF~*(B)的发射谱,没有观察到CH~*及CHF~*.结合以前的激光诱导荧光实验结果,通过化学热力学分析,借助中间络合物形成机制,我们解释了实验观察到的所有现象。     

Cl+F2→ClF+F和F+ClF′→ClF+F′反应机理的密度泛函理论研究

用密度泛函理论(DFT)B3LYP方法, 在6-311G基组下,计算研究了反应Cl+F2→ClF+F和对称反应F+ClF′→ClF+F′的机理。求得前者的过渡态为三角形,活化能为15.57 kJ*mol-1;后者的过渡态为线形和三角形,活化能分别为11.52和196.25 kJ*mol-1。结果均经过振动分析和IRC计算验证。     

The visible chemiluminescence of the reaction F + CH3F

By using molecular beam apparatus the visible (450–900 nm) chemiluminescence of the reaction F + CH₃F was investigated. Seven vibronic bands of HCF (Ã₁A-XA') and four vibrational bands of HF ground state overtone transitions were obtained. The relative vibrational state distributions of HF (V'=4,5,6) states and the rotational temperature of HF (V'=3) state were obtained. The analyses show that the two kinds of spectra were caused by the secondary reaction F+CH₃F. The results may be helpful to explain the contradictory results of the experiments in F+CH₃F system.     

Infrared laser spectroscopy of CH3...HF in helium nanodroplets: The exit-channel complex of the F + CH4 reaction

High-resolution infrared laser spectroscopy is used to study the CH3...HF and CD3...HF radical complexes, corresponding to the exit-channel complex in the F + CH4 --> HF + CH3 reaction. The complexes are formed in helium nanodroplets by sequential pickup of a methyl radical and a HF molecule. The rotationally resolved spectra presented here correspond to the fundamental v = 1 <-- 0 H-F vibrational band, the analysis of which reveals a complex with C(3v) symmetry. The vibrational band origin for the CH3...HF complex (3797.00 cm(-1)) is significantly redshifted from that of the HF monomer (3959.19 cm(-1)), consistent with the hydrogen-bonded structure predicted by theory [E. Ya. Misochko et al., J. Am. Chem. Soc. 117, 11997 (1995)] and suggested by previous matrix isolation experiments [M. E. Jacox, Chem. Phys. 42, 133 (1979)]. The permanent electric dipole moment of this complex is experimentally determined by Stark spectroscopy to be 2.4+/-0.3 D. The wide amplitude zero-point bending motion of this complex is revealed by the vibrational dependence of the A rotational constant. A sixfold reduction in the line broadening associated with the H-F vibrational mode is observed in going from CH3...HF to CD3...HF. The results suggest that fast relaxation in the former case results from near-resonant intermolecular vibration-vibration (V-V) energy transfer. Ab initio calculations are also reported (at the MP2 level) for the various stationary points on the F + CH4 surface, including geometry optimizations and vibrational frequency calculations for CH3...HF.     

Molecular elimination in photolysis of o- and p-fluorotoluene at 193 nm: Internal energy of HF determined with time-resolved Fourier transform spectroscopy

Following the photodissociation of o-fluorotoluene [o-C(6)H(4)(CH(3))F] at 193 nm, rotationally resolved emission spectra of HF(1< or =v< or =4) in the spectral region of 2800-4000 cm(-1) are detected with a step-scan Fourier transform spectrometer. HF(v< or =4) shows nearly Boltzmann-type rotational distributions corresponding to a temperature approximately 1080 K; a short extrapolation from data in the period of 0.5-4.5 mus leads to a nascent rotational temperature of 1130+/-100 K with an average rotational energy of 9+/-2 kJ mol(-1). The observed vibrational distribution of (v=1):(v=2):(v=3)=67.6: 23.2: 9.2 corresponds to a vibrational temperature of 5330+/-270 K. An average vibrational energy of 25+/-(3) (12) kJ mol(-1) is derived based on the observed population of HF(1< or =v< or =3) and estimates of the population of HF (v=0 and 4) by extrapolation. Experiments performed on p-fluorotoluene [p-C(6)H(4)(CH(3))F] yielded similar results with an average rotational energy of 9+/-2 kJ mol(-1) and vibrational energy of 26+/-(3) (12) kJ mol(-1) for HF. The observed distributions of internal energy of HF in both cases are consistent with that expected for four-center elimination. A modified impulse model taking into account geometries and displacement vectors of transition states during bond breaking predicts satisfactorily the rotational excitation of HF. An observed vibrational energy of HF produced from fluorotoluene slightly smaller than that from fluorobenzene might indicate the involvement of seven-membered-ring isomers upon photolysis.     

Comparison of experimental time-of-flight spectra of the HF products from the F+H2 reaction with exact quantum mechanical calculations

High resolution HF product time-of-flight spectra measured for the reactive scattering of F atoms from n-H2(p-H2) molecules at collision energies between 69 and 81 meV are compared with exact coupled-channel quantum mechanical calculations based on the Stark-Werner ab initio ground state potential energy surface. Excellent agreement between the experimental and computed rotational distributions is found for the HF product vibrational states v'=1 and v'=2. For the v'=3 vibrational state the agreement, however, is less satisfactory, especially for the reaction with p-H2. The results for v'=1 and v'=2 confirm that the reaction dynamics for these product states is accurately described by the ground electronic state 1 (2)A' potential energy surface. The deviations for HF(v'=3, j' > or =2) are attributed to an enhancement of the reaction resulting from the 25% fraction of excited ((2)P(12)) fluorine atoms in the reactant beam.     

用交叉束激光诱导荧光技术研究氟原子与碘化物的反应

在570-620 nm波长范围内用交叉束激光诱导荧光技术研究了F原子与C_2H_5I, C_2F_5I和C_3H_5I的反应, 获得了反应产物IF的振功和转功激发谱; 测得了反应产物IF在v=3, 4和5能级中的初生相对振动布居密度, 和部分的相对细致振动速率常数, 转动温度和振功能级中转动能量的平均部分数; 并对反应机制进行了讨论。     

Nonadiabatic reactant-product decoupling calculation for the F(2P(1/2)) + H2 reaction

In this paper we present a theoretical study using time-dependent nonadiabatic reactant-product decoupling method for the state-to-state reactive scattering calculation of F((2)P(1/2))+H(2) (nu=j=0) reaction on the Alexander-Stark-Werner potential energy surface. In this nonadiabatic state-to-state calculation, the full wave function is partitioned into reactant component and a sum of all product components. The reactant and product components of the wave function are solved independently. For the excited state reaction, the state-to-state reaction probabilities for J=0.5 are calculated. Comparing the state-to-state reaction probabilities, it is found that the vibrational population of the HF product is dominated by vibrational levels nu=2 and 3. The rotation specific reaction probabilities of HF product in j=1 and 2 are larger than those in other rotational levels. As the rotation quantum number j increases, the positions of the peak in the rotational reaction probability of HF product in nu=3 shift to higher collision energy.     

The OsO4F-, OsO4F2(2)-, and OsO3F3- anions, their study by vibrational and NMR spectroscopy and density functional theory calculations, and the X-ray crystal structures of [N(CH3)4][OsO4F] and [N(CH3)4][OsO3F3

The fluoride ion acceptor properties of OsO4 and OsO3F2 were investigated. The salts [N(CH3)4][OsO4F] and [N(CH3)4]2[OsO4F2] were prepared by the reactions of OsO4 with stoichiometric amounts of [N(CH3)4][F] in CH3CN solvent. The salts [N(CH3)4][OsO3F3] and [NO][OsO3F3] were prepared by the reactions of OsO3F2 with a stoichiometric amount of [N(CH3)4][F] in CH3CN solvent and with excess NOF, respectively. The OsO4F- anion was fully structurally characterized in the solid state by vibrational spectroscopy and by a single-crystal X-ray diffraction study of [N(CH3)4][OsO4F]: Abm2, a = 7.017(1) A, b = 11.401(2) A, c = 10.925(2) A, V = 874.1(3) A3, Z = 4, and R = 0.0282 at -50 degrees C. The cis-OsO4F2(2-) anion was characterized in the solid state by vibrational spectroscopy, and previous claims regarding the cis-OsO4F2(2-) anion are shown to be erroneous. The fac-OsO3F3- anion was fully structurally characterized in CH3CN solution by 19F NMR spectroscopy and in the solid state by vibrational spectroscopy of its N(CH3)4+ and NO+ salts and by a single-crystal X-ray diffraction study of [N(CH3)4][OsO3F3]: C2/c, a = 16.347(4) A, b = 13.475(3) A, c = 11.436(3) A, beta = 134.128(4) degrees, V = 1808.1(7) A3, Z = 8, and R = 0.0614 at -117 degrees C. The geometrical parameters and vibrational frequencies of OsO4F-, cis-OsO4F2(2-), monomeric OsO3F2, and fac-OsO3F3- and the fluoride affinities of OsO4 and monomeric OsO3F2 were calculated using density functional theory methods.     

Molecular elimination in photolysis of fluorobenzene at 193 nm: internal energy of HF determined with time-resolved Fourier-transform spectroscopy

Following photodissociation of fluorobenzene (C(6)H(5)F) at 193 nm, rotationally resolved emission spectra of HF(1相似文献   

Ar、NO和CHBr3对电子激发态CH的淬灭

The collisional quenching rate constants of CH(A, V'=0) by Ar and CHBr_3 and CH(A, B, V'=0) by NO molecule were measured by means of laser photolysis of CHBr_3 molecule at 266 nm generating CH(A, B) radicals and monitoring the time-resolved signal of ethession CH(A, B→X). The dependence of quenching rate constant of CH(A, V'=0) by CHBr_3 on rotational state of CH(A) is presented. It is found that the quenching rate decreases with increasing rotational quantum number of CH(A).