CH_3N_3的光解─生成三线态CH_3N自由基的光谱证据(英文)

研究了CH3N3在第一电子吸收带的光解，获得了生成三线态CH3N自由基的重要证据并对可能的反应机制进行了讨论．其机理以激发态CH3N3经单线态三线态相互作用后解离生成三线态自由基的可能性较大．     

à 3E态CH3N自由基的稳定性

观察到了CH_3N自由基Ã ~3E←X~3A_2体系317-272 nm的荧光激发谱, 特别讨论了振动激发的Ã 态的稳定性. 报导了v_3~′=6态的色散荧光和荧光时间谱, 该态在240 Pa下的寿命大约是80 ns. 实验表明Ã ~3E 态CH_3N自由基是稳定的, 势能面至少距振动基态4800 cm~(-1)内是束缚的, 异构化或预离解作用并不重要.     

CH自由基共振增强多光子电离光谱

ＣＨ自由基在燃烧化学、星际化学、化学发光和化学激光研究中占有重要的地位,并且作为最简单的碳氢化合物,ＣＨ自由基是理想的理论计算模型分子,在理论研究领域中也有着重要的地位．因此 ,多年来人们对ＣＨ自由基进行了大量的研究［１ -９］,但是对于ＣＨ自由基,到目前为止大部分局限于低激发态的研究,对于较高激发态的研究报导则很少见．Ｃｈｕｐｋａ等［２ -６］用(２ １)ＲＥＭＰＩ方法获得了ＣＨＤ态的ｖ＝２振动能级光谱．然而后来Ｔｊｏｓｓｅｍ和Ｓｍｙｔｈ［７］测量了同波段的ＲＥＭＰＩ光谱,发现他们测得的光谱谱峰强度与…     

氯代烃光解活泼自由基的ESR研究

本文用2,4-二硝基苯亚甲基特丁基氮氧化物(DNPBN)作自由基捕捉剂研究了氯代烃光解过程产生的自由基中间体。实验结果表明在汞灯照射下键能较低的多氯代烷烃分子中的碳-氯键极易发生均裂而产生碳中心自由基与活泼的氯原子, 并且后者可被DNPBN捕获, 形成颇为稳定的氮氧自由基加合物[Cl-DNPBN]~·。对多氯代苯,随着取代氯原子数目增多, 加合物[Cl-DNPBN]~·的ESR信号强度也明显增加。此外, DNPBN对氯原子的大量捕捉实验还证明它对氯原子是一种高效的特征捕捉剂。     

光解苯半醌和2-羟基-2-丙基自由基的CIDEP谱

用高时间分辨ＥＳＲ波谱仪测量了光解苯半醌和２－羟基－２－丙基自由基的ＣＩＤＥＰ谱,苯半醌自由基的ＣＩＤＥＰ属ＴＭ机理,实验研究了微波功率,溶液浓度对苯半醌自由基的ＣＩＤＥＰ谱时间演化的影响,２－羟基－２－丙基自由基的ＣＩＤＥＰ属ＲＰＭ机理,实验研究了自旋极化的生成环境。     

~3E态CH_3N自由基的稳定性(英文)

观察到了CH_3N自由基~3E←~3A_2体系317-272nm 的荧光激发谱,特别讨论了振动激发的态的稳定性.报导了v_3~′=6态的色散荧光和荧光时间谱,该态在240 Pa 下的寿命大约是80ns.实验表明~3E 态CH_3N 自由基是稳定的,势能面至少距振动基态4800 cm~(-1)内是束缚的,异构化或预离解作用并不重要.     

有机锡化合物光解活泼自由基的ESR研究

本文用自旋捕捉技术与ESR相结合的方法,研究了六种有机锡化合物的光解反应历程。结果表明:有机锡化合物紫外光照时,碳-锡键发生均裂,产生碳中心和锡中心自由基。其中碳中心自由基易被捕捉剂α-苯基-N-特丁基氮氧化物(PBN)或2,3,5,6-四甲基亚硝基苯(ND)所捕获;而锡中心自由基可与菲醌形成稳定的环状加合物。由于环状加合物中配体的不同,产生的空间效应也不同,从而导致加合物中的未偶电子云密度发生变化,给出相异的ESR信号。     

苯甲醛及对溴苯甲醛光解初级过程自由基的ESR研究

苯甲醛的光解与其在放置过程中的自氧化引发机理密切相关,因此确定光解过程的主要中间产物有重要意义。自氧化的全过程比较复杂,但单纯的光解本身显然相对简单一些。本文用自旋捕捉-ESR技术研究了苯甲醛及与其相类似的对溴苯甲醛在紫外和可见光作用下生成的活泼中间体,并讨论了在本文实验条件下的光解初级过程。     

激光光解苯醌自由基质子交换的TRESR研究

用时间分辨电子自旋共振（TRESR）波谱仪，研究了对苯醌/乙二醇/水体系中激光光解苯醌自由基的TRESR谱的线形与溶液pH值的关系.实验表明TRESR谱线均为发射极极化，极化过程以三重态机理（TM）为主.在中性溶液中谱线属中性苯半醌自由基BQH•,而在pH～2.02酸性溶液中谱线属阳离子基BQH＋.实验发现 BQH＋的TRESR谱强度的衰减具有超精细分量相关性，用质子交换理论对此进行了解释.     

电子激发态CH（C^2Σ^＋）自由基的猝灭速率常数的测定

用２６６ｎｍ激光光解ＣＨＢｒ３分子产生ＣＨ（Ｃ）态自由基，通过测量ＣＨ（Ｃ＾２Σ＾＋→Ｘ＾２Ⅱ）的总荧光信号强度来测定室温下Ｏ２、Ｎ２、ｎ－Ｃ５Ｈ１２、ｎ－Ｃ６Ｈ１４和ｎ－Ｃ７Ｈ１６对ＣＨ（Ｃ２Σ＾＋，ｖ′＝０）的猝灭常数。结果表明，这些碰撞伴侣（Ｏ２和Ｎ２例外）对ＣＨ（Ｘ、Ａ、Ｂ和Ｃ）的反应或猝灭速率常数ｋ存在下列关系：ｋ（Ｘ）〉ｋ（Ｂ）〉ｋ（Ａ）≈ｋ（Ｃ），且烷烃分子对ＣＨ（Ｃ）态的猝灭速率常     

Photodissociation Study of Ca+-Dipropylamine Complex

Gas-phase Ca⁺-dipropylamine complex has been subjected to photodissociation (400-690 nm). One reactive product, Ca⁺-NHC₃H₇, is detected only in the region of 450-528 nm, besides the evaporation fragment of Ca⁺, which is dominant throughout the whole spectral region we have studied. The photoreaction channel may be explained in terms of a metal insertion mechanism. The calculated results are in good agreement with the experimental observations.     

Theoretical Investigations on Photodissociation Dynamics of Deuterated Alkyl Halides CD3CH2F

The product branching ratio between different products in multichannel reactions is as important as the overall rate of reaction, both in terms of practical applications (\emph{e.g}. models of combustion or atmosphere chemistry) in understanding the fundamental mechanisms of such chemical reactions. A global ground state potential energy surface for the dissociation reaction of deuterated alkyl halide CD\begin{document}$ _3 $\end{document}CH\begin{document}$ _2 $\end{document}F was computed at the CCSD(T)/CBS//B3LYP/aug-cc-pVDZ level of theory for all species. The decomposition of CD\begin{document}$ _3 $\end{document}CH\begin{document}$ _2 $\end{document}F is controversial concerning C\begin{document}$ - $\end{document}F bond dissociation reaction and molecular (HF, DF, H\begin{document}$ _2 $\end{document}, D\begin{document}$ _2 $\end{document}, HD) elimination reaction. Rice-Ramsperger-Kassel-Marcus (RRKM) calculations were applied to compute the rate constants for individual reaction steps and the relative product branching ratios for the dissociation products were calculated using the steady-state approach. At the different energies studied, the RRKM method predicts that the main channel for DF or HF elimination from 1, 2-elimination of CD\begin{document}$ _3 $\end{document}CH\begin{document}$ _2 $\end{document}F is through a four-center transition state, whereas D\begin{document}$ _2 $\end{document} or H\begin{document}$ _2 $\end{document} elimination from 1, 1-elimination of CD\begin{document}$ _3 $\end{document}CH\begin{document}$ _2 $\end{document}F occurs through a direct three-center elimination. At 266, 248, and 193 nm photodissociation, the main product CD\begin{document}$ _2 $\end{document}CH\begin{document}$ _2 $\end{document}+DF branching ratios are computed to be 96.57%, 91.47%, and 48.52%, respectively; however, at 157 nm photodissociation, the product branching ratio is computed to be 16.11%. Based on these transition state structures and energies, the following photodissociation mechanisms are suggested: at 266, 248, 193 nm, CD\begin{document}$ _3 $\end{document}CH\begin{document}$ _2 $\end{document}F\begin{document}$ \rightarrow $\end{document}absorption of a photon\begin{document}$ \rightarrow $\end{document}TS5\begin{document}$ \rightarrow $\end{document}the formation of the major product CD\begin{document}$ _2 $\end{document}CH\begin{document}$ _2 $\end{document}+DF; at 157 nm, CD\begin{document}$ _3 $\end{document}CH\begin{document}$ _2 $\end{document}F\begin{document}$ \rightarrow $\end{document}absorption of a photon\begin{document}$ \rightarrow $\end{document}D/F interchange of TS1\begin{document}$ \rightarrow $\end{document}CDH\begin{document}$ _2 $\end{document}CDF\begin{document}$ \rightarrow $\end{document}H/F interchange of TS2\begin{document}$ \rightarrow $\end{document}CHD\begin{document}$ _2 $\end{document}CHDF\begin{document}$ \rightarrow $\end{document}the formation of the major product CHD\begin{document}$ _2 $\end{document}+CHDF.     

Photodissociation of CH3Cl+ and CH3Br+ in a tandem quadrupole mass spectrometer

A new tandem quadrupole photodissociation mass spectrometer was used to measure photodissociation cross sections for the reactions, CH₃Cl⁺ → CH₃⁺ + Cl and CH₃Br⁺ → CH₃⁺ + Br in the gas phase using wavelength-selected light. The results on CH₃Cl⁺ are compared with the earlier work of Dunbar. For both reactions we are able to observe photodissociations occurring with small cross sections (≈ 2 × 10^?20 cm²) in the visible region near the thermochemical thresholds.     

Photodissociation spectrum of CH3I+ prepared by multiphoton ionization

Two-photon resonant multiphoton ionization has been used to prepare rotationally cooled and selected CH₃I⁺ ions with controlled vibrational and electronic distributions. These ions are photodissociated by a second laser. The highly simplified photodissociation spectrum displays a clear dissociation threshold as well as bands hidden in earlier spectra. The data suggests corrections to previously determined vibrational constants.     

Investigation on the Photodissociation of Oxygen from Oxymyoglobin by Fluorescence Spectroscopy

Photodissociation of oxygen from oxymyoglobin(oxyMb) was investigated by means of fluorescence spectroscopy. One of the most important findings of the photodissociation of oxyMb was the discovery of two processes which were affected by excitation intensity, temperature, solvent viscosity, and excitation wavelength. Process I(PI) corresponded to oxygen escaping from the binding site at ferrous heme iron atom within the porphyrin ring into the heme pocket, whereas process II(PII) was ascribed to oxygen escaping from the heme pocket into the solvent. To elucidate this interesting phenomenon, we proposed a model that oxygen encountered two barriers on its way from the binding site at the ferrous heme iron to the solvent. Reversibility and wavelength sensitivity of the photodissociation were also observed.     

Detection of OH Radical in the Photodissociation of p-Aminobenzoic Acid at 266 nm

Photodissociation of p-aminobenzoic acid at 266 nm was investigated by probing the nascent OH photoproduct employing the laser-induced fluorescence technique. It was found that the nascent OH radical was vibrationally cold and its rotational state distribution conformed to be a Boltzmann behavior, characterized by a rotational temperature of 1040±110 K. The rotational energy of OH was determined to be 8.78±0.84 kJ/mol. Between the two spinorbit states of OH, ^2Ⅱ3/2 and ^2Ⅱ1/2, the former was found to be preferentially populated. The distribution of the II（A＇） state for the A-doublet was dominant. Finally, a probable mechanism for the formation of OH produced from the photodissociation of p-aminobenzoic acid is discussed.     

AIM Study on the Reaction of CH2SH Radical with Fluorine Atom

The reaction of CH2SH radical with fluorine atom was studied at the levels of B3LYP/6-311G(d,p) and MP2(Full)/6-311G(d,p). The computational results show that the reaction has three channels and proceeds by the addition of fluorine atoms on carbon or sulfur sites of CH2SH, forming initial intermediates. The calculated results show that the channel in which fluorine attaches to the carbon atom to form CH2S and HF, is the most likely reaction pathway. Topological analysis of electron density was carried out for the three channels. The change trends of the chemical bonds on the reaction paths were discussed. The energy transition states and the structure transition regions (states) of the three channels were found. The calculated results show that the structure transition regions are broad in unobvious exothermic reactions or unobvious endothermic reactions, and are narrow in obvious exothermic reactions or obvious endothermic reactions.     

CS2+离子 C2Σg+←B2Σu+跃迁的Franck-Condon因子计算以及与光解离谱的比较

将线性三原子分子离子CS2+的对称伸缩振动简化为SC和S之间的简谐振动, 用谐振子的势能曲线和波函数对CS2+分子离子 C2Σg+和 B2Σu+电子态(对称伸缩)振动能级间跃迁的Franck-Condon因子进行了计算, 得到的结果与 C2Σg+←B2Σu+跃迁的光解离谱实验强度进行了比较, 对前人给出的分子数据(转动常数、分子平衡核间距)进行了验证和分析, 讨论了经由 C2Σg+←B2Σu+电子态振动能级间跃迁的光解离机理.     

Softening of C-H Symmetric Stretching Vibrational Modes for CH2 and CH3 Radicals Adsorbed on Cun (n=1-6) Clusters

The properties of C-H vibration softening for CH₂ and CH₃ radicals absorbed on Cu_n(n=1-6) clusters have been investigated, using the density functional theory with hybrid functional. The results indicate that the absorption of CH₂ on Cu clusters is stronger than the case of CH₃. The vibrational frequencies of C-H bonding agree with the experimental results obtained for CH₂ and CH₃ absorbed on Cu(111). With the increase of cluster size, the softening (Einstein shift) of C-H vibrational modes become stronger.     

HOD分子在(~C)1B1态的光解动力学:产物OH/OD的分支比以及OD键解离能

Photodissociation of jet-cooled HOD via the ? state around 124 nm has been studied using the H(D)-atom Rydberg tagging time-of-flight technique. Rotational state resolved action spectrum and the product translational energy distribution spectra have been recorded for both D+OH and H+OD dissociation channels. Product channel OH/OD branching ratios for the individual ?- X rotational transition have been determined. A comparison is also given with the B- X and ?- X transitions. In addition, the dissociation energy of the OD bond in HOD has been determined accurately to be 41751.3±5 cm^-1.