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1.
采用半经典动力学方法模拟了5-甲基胞嘧啶(5m-Cyt)和胞嘧啶(Cyt)在267 nm紫外光辐射下的光物理失活过程. 模拟发现, 5m-Cyt 和Cyt 的激发态通过C5-C6键的扭曲以及甲基(或H5)和H6原子平面外振动失活.失活时, 甲基(或H5)和H6原子几乎与环面垂直并指向不同方向, 形成“双自由基态”. 由于甲基的体积比H原子的大, 振动频率较小, 使得C5原子的变形受到抑制, 导致5m-Cyt 的激发态寿命比胞嘧啶更长. 完全活性空间自洽场(CASSCF)计算显示, 5m-Cyt的圆锥交叉(CI)点能量比Cyt 高0.3 eV, 这也证明5m-Cyt演化至CI 需要克服更大的能垒, 因此激发态寿命长于胞嘧啶.  相似文献   

2.
采用半经典电子-辐射-离子动力学(SERID)模型模拟了π堆积的腺嘌呤-胸腺嘧啶(A-T)体系激发态的光物理失活过程. 设置激光脉冲仅作用于T, 模拟发现电子由A转移到T, 形成(A+T-)*激基缔合物(exciplex). 当分子间距缩短至0.300 nm时, 由于轨道离域效应产生电荷重组, 体系恢复电中性; 当A分子的C4'-C5'扭曲程度最大时, 体系通过避免交叉点衰减至基态. Exciplex 的失活途径由分子间距离和A分子的变形程序两个因素决定. 由于A分子的C4'、C5'原子位阻较大, 难以达到失活所必需的强烈扭曲, 因此(A-T)*的寿命比胸腺嘧啶堆积体系(T-T)*显著增长.  相似文献   

3.
利用时间分辨的飞秒光电子影像技术结合时间分辨的质谱技术, 研究了2-氯吡啶分子激发态的超快过程. 实时观察到了2-氯吡啶分子第二激发态(S2)向第一激发态(S1)高振动能级的的超快内转换过程,该内转换的时间常数为(162±5)fs. 实验结果表明, 通过S2/S0的锥形交叉衰减到基态的衰减通道也是退布居的重要通道, 其时间尺度为(5.5±0.3) ps.  相似文献   

4.
噻吩光解反应机理的理论研究   总被引:1,自引:0,他引:1  
使用密度泛函理论(DFT)中的B3LYP方法, 采用6-31G**和6-31++G**基组, 对噻吩的光解反应进行了理论研究. 对照实验结果, 我们研究了五个光解通道, 包括生成C4H4+S, C2H2+C2H2S和CS+C3H4的三个闭壳层分子解离通道与生成HCS+C3H3和HS+C4H3的自由基解离通道. 各个可能的反应通道的产物碎片的具体形式得到了确认. 研究发现在基态生成C2H2+C2H2S和在最低三态生成C4H4+S的反应从能量上考虑最为有利, 而实验上观测到的主要产物C2H2+C2H2S主要是在基态上产生的. 通过对比实验结果与计算结果, 我们认为噻吩光解反应机理与所用激发光波长有关.  相似文献   

5.
以Cu+和Zn+与CS2反应作为第一过渡金属离子与CS2反应的范例体系. 采用密度泛函UB3LYP/6-311+G*方法计算研究了第一过渡金属离子在基态和激发态与CS2反应的反应机理. 全参数优化了反应势能面上各驻点的几何构型, 用频率分析方法和内禀反应坐标(IRC)方法对过渡态进行了验证. 并用UCCSD(T)/6-311G*方法对各驻点作了单点能量校正. 在Cu+与CS2反应中, 计算了单重态初始中间体1IM1到三重态插入型中间体3IM2的反应交叉势能面. 确定了第一过渡金属离子与CS2的反应为插入-消去反应, 找到了基态和激发态金属离子与CS2反应的主要通道.  相似文献   

6.
王树建  李莹  吴迪* 《物理化学学报》2012,28(12):2817-2823
采用二级微扰理论(MP2)量子化学研究方法, 对C2H4-nFn···LiH (n=0, 1, 2)二聚体的结构和π锂键性质进行了分析. 结果表明氟原子的取代改变了乙烯分子的π电子云形状, 从而使二聚体体系中的π锂键发生偏移、伸长和弯曲. 通过与类似的π氢键体系C2H4-nFn···HF (n=0, 1, 2)比较, 发现π锂键在二级弱相互作用的影响下, 发生了明显的弯曲, 表现出弱的方向性. 在CCSD(T)/6-311++G(3df, 3pd)理论水平下, 二聚体的相互作用能强弱顺序为: 33.85 kJ·mol-1 (C2H4-LiH)>27.32 kJ·mol-1 (C2H3F-LiH)>21.34 kJ·mol-1 (cis-C2H2F2-LiH)>20.25 kJ·mol-1 (g-C2H2F2-LiH), 说明氟取代削减了乙烯分子与LiH之间的相互作用.  相似文献   

7.
以Cu+和Zn+与CS2反应作为第一过渡金属离子与CS2反应的范例体系. 采用密度泛函UB3LYP/6-311+G*方法计算研究了第一过渡金属离子在基态和激发态与CS2反应的反应机理. 全参数优化了反应势能面上各驻点的几何构型, 用频率分析方法和内禀反应坐标(IRC)方法对过渡态进行了验证. 并用UCCSD(T)/6-311G*方法对各驻点作了单点能量校正. 在Cu+与CS2反应中, 计算了单重态初始中间体1IM1到三重态插入型中间体3IM2的反应交叉势能面. 确定了第一过渡金属离子与CS2的反应为插入-消去反应, 找到了基态和激发态金属离子与CS2反应的主要通道.  相似文献   

8.
合成了钌(II)配合物cis-[Ru(HL)(Hdcbpy)(NCS)2]•[N(C4H9)4](HL=2-(9-乙基-9H-3-咔唑基)-1H-咪唑[4,5-f] [1,10]邻菲啰啉, H2dcbpy=4,4'-二羧酸-2,2'-联吡啶). 采用元素分析、核磁共振氢谱、红外光谱、紫外-可见吸收光谱、质谱(MS)对配合物进行了表征. 通过紫外-可见吸收光谱和稳态荧光光谱, 研究了该配合物的基态和激发态酸碱性质. 结果表明该配合物在基态时能发生5步质子化/去质子化反应, 表现出基于光致发光强度和激发态能量转移途径的质子化/去质子化诱导的分子开关性质.  相似文献   

9.
密度泛函理论研究十二烷硫醇在Au(111)面上的吸附   总被引:1,自引:0,他引:1  
采用第一性原理方法研究了十二烷硫醇(C12H25SH)分子在Au(111)面上未解离和解离吸附的结构、能量和吸附性质,在此基础上分析判断长链硫醇分子在Au(111)面吸附时S―H键的解离, 以及分子链长度对吸附结构和能量的影响. 计算了S原子在不同位置以不同方式吸附的系列构型, 结果表明在S―H键解离前和解离后,均存在两种可能的表面结构, 直立吸附构型和平铺吸附构型; 未解离的C12H25SH分子倾向于吸附在top位, 吸附能为0.35-0.38 eV; H原子解离后C12H25S基团倾向于吸附在bri-fcc位, 吸附能量为2.01-2.09 eV. 比较分析未解离吸附和解离吸附, 发现C12H25SH分子未解离吸附相较于解离吸附要稳定, 未解离吸附属于弱化学吸附.局域电子态密度和差分电荷密度分析进一步验证了S―H解离后S原子与表面之间成键的数目增加, 而且键合更强. 同时我们发现长链硫醇的吸附能量较短链硫醇的吸附能量略大, S原子与表面Au原子之间的距离略小.  相似文献   

10.
甘雄  谢音  任小明  沈玉芳  彭正合  周运鸿 《化学学报》2005,63(14):1307-1312
测量了标题配合物Ni(mnt)(phen)在多种介质中的电子吸收光谱和发射光谱, 使用密度泛函理论的B3LYP方法和分子轨道理论的PM3方法研究了其气态分子几何构型、电子结构和成键, 用ZINDO/S方法通过多组态的组态相互作用(CI)计算解释了实验光谱. 结果表明: 该配合物分子为平面结构, 对称性属于点群C2v, 基态为自旋三重态, 配位键Ni—N和Ni—S为典型的共价结合, Ni的3d电子反馈效应较显著; 可见区的吸收带和发射带(对应于基态电子组态到较低能量激发态组态的跃迁)本质上属于配体phen到mnt2-的荷移跃迁(LL'CT), 紫外区的吸收带本质上属于配体的π→π*跃迁.  相似文献   

11.
The nonradiative decay of a π-stacked pair of adenine molecules,one of which was excited by an ultrafast laser pulse,is studied by semiclassical dynamics simulations.This simulation investigation is focused on the effect of the formation of bonded excimer in stacked adenines on the mechanism of ultrafast decay.The simulation finds that the formation of the bonded excimer significantly lowers the energy gap between the LUMO and HOMO and consequently facilitates the deactivation of the electronically excited molecule.On the other hand,the formation of the chemical bond between two stacked adenines restricts the deformation vibration of the pyrimidine of the excited molecule due to the steric effect.This slows down the formation of the coupling between the HOMO and LUMO energy levels and therefore delays the deactivation process of the excited adenine molecule to the electronic ground state.  相似文献   

12.
采用半经典动力学方法模拟了π堆积的胸腺嘧啶体系最低激发态的光物理失活过程.设置激光脉冲仅作用于一个胸腺嘧啶分子T,另一胸腺嘧啶分子T’保持基态.模拟发现由于T与T’之间存在π堆积相互作用,导致电荷转移,形成T带负电荷、T’带正电符的激基复合物.由于相邻分子的空间效应阻碍了激发的T分子到达圆锥相交所必需的强烈扭曲,激基复合物的寿命比单体增长.当分子间距离缩短至0.3 nm后,T分子C5—C6键扭曲程度最大,此时发生电荷重组,两个胸腺嘧啶分子均恢复电中性.电荷重组诱导T’分子发生畸变,并在C5’—C6’扭曲最大时避免相交,体系衰减至基态,T和T’分子均恢复平面构型.  相似文献   

13.
A realistic dynamics simulation study is reported for the ultrafast radiationless deactivation of 9H-adenine. The simulation follows two different excitations induced by two 80 fs (fwhm) laser pulses that are different in energy: one has a photon energy of 5.0 eV, and the other has a photon energy of 4.8 eV. The simulation shows that the excited molecule decays to the electronic ground state from the (1)pipi* state in both excitations but through two different radiationless pathways: in the 5.0 eV excitation, the decay channel involves the out-of-plane vibration of the amino group, whereas in the 4.8 eV excitation, the decay strongly associates with the deformation of the pyrimidine at the C 2 atom. The lifetime of the (1) npi* state determined in the simulation study is 630 fs for the 5.0 eV excitation and 1120 fs for the 4.8 eV excitation. These are consistent with the experimental values of 750 and 1000 fs. We conclude that the experimentally observed difference in the lifetime of the (1) npi* state at various excitations results from the different radiationless deactivation pathways of the excited molecule to the electronic ground state.  相似文献   

14.
We report quantum dynamical simulations for the laser controlled isomerization of 1-(2-cis-fluoroethenyl)-2-fluorobenzene based on one-dimensional electronic ground and excited state potentials obtained from (TD)DFT calculations. 1-(2-cis-fluoroethenyl)-2-fluorobenzene supports two chiral and one achiral atropisomers, the latter being the most stable isomer at room temperature. Using a linearly polarized IR laser pulse the molecule is excited to an internal rotation around its chiral axis, i.e. around the C-C single bond between phenyl ring and ethenyl group, changing the molecular chirality. A second linearly polarized laser pulse stops the torsion to prepare the desired enantiomeric form of the molecule. This laser control allows the selective switching between the achiral and either the left- or right-handed form of the molecule. Once the chirality is "switched on" linearly polarized UV laser pulses allow the selective change of the chirality using the electronic excited state as intermediate state.  相似文献   

15.
Relaxation of highly vibrationally excited pyrimidine (C(4)N(2)H(4)) by collisions with carbon dioxide has been investigated using diode laser transient absorption spectroscopy. Vibrationally hot pyrimidine (E(')=40 635 cm(-1)) was prepared by 248-nm excimer laser excitation, followed by rapid radiationless relaxation to the ground electronic state. The nascent rotational population distribution (J=58-80) of the 00(0)0 ground state of CO(2) resulting from collisions with hot pyrimidine was probed at short times following the excimer laser pulse. Doppler spectroscopy was used to measure the CO(2) recoil velocity distribution for J=58-80 of the 00(0)0 state. Rate constants and probabilities for collisions populating these CO(2) rotational states were determined. The measured energy transfer probabilities, indexed by final bath state, were resorted as a function of DeltaE to create the energy transfer distribution function, P(E,E(')), from E(')-E approximately 1300-7000 cm(-1). P(E,E(')) is fitted to a single exponential and a biexponential function to determine the average energy transferred in a single collision between pyrimidine and CO(2) and parameters that can be compared to previously studied systems using this technique, pyrazineCO(2), C(6)F(6)CO(2), and methylpyrazineCO(2). P(E,E(')) parameters for these four systems are also compared to various molecular properties of the donor molecules. Finally, P(E,E(')) is analyzed in the context of two models, one which suggests that the shape of P(E,E(')) is primarily determined by the low-frequency out-of-plane donor vibrational modes and one which suggests that the shape of P(E,E(')) can be determined by how the donor molecule final density of states changes with DeltaE.  相似文献   

16.
The single crystal X-ray diffraction structure of 2-(2′-pyridylthio)-3-nitropyridine is reported. A non-bonded interaction was observed between the sulfur atom and one of the oxygen atoms of the nitro group with an interatomic distance of 2.678 A. Examination of the molecule's behavior in solution by 13C-nmr spin-lattice (T1) relaxation measurements showed the non-nitro bearing pyridyl ring to reorient anisotropically about the C2′-C5′ bond axis. In contrast, the nitro substituted pyridine ring did not appear to exhibit anisotropic reorientation about the corresponding C2-C5 bond axis. Rather, approximately equivalent relaxation times were noted for all protonated ring carbons, indicating that the relaxations of this portion of the molecule were governed by the overall isotropic reorientation of the system. Based on these observations, it was concluded that the intramolecular sulfur-nitro interaction also operates in the solution state and is sufficiently strong to prevent free rotation of the substituted portion of the molecule about the C2-S bond axis.  相似文献   

17.
The title compound undergoes efficient photoaddition of a molecule of a hydroxylic solvent (H(2)O, MeOH, (Me)(2)CHOH) across the 9- and 10-positions of the anthracene moiety to give isolable triphenylmethanol or triphenylmethyl ether type products. The reaction is believed to proceed via a mechanism involving water-mediated formal excited state intramolecular proton transfer (ESIPT) from the phenolic OH to the 10-position of the anthracene ring, generating an o-quinone methide intermediate that is observable by nanosecond laser flash photolysis, and is trappable with nucleophiles. A "water-relay" mechanism for proton transfer seems plausible but cannot be proven directly with the data available. Irradiation in deuterated solvents led to incorporation of one deuterium atom at the methylene position in the photoaddition product, and partial deuterium exchange of the 10-position of recovered starting material, consistent with the proposed formal excited state proton transfer mechanism. The deuterium exchange and photoaddition reach maximum quantum efficiency at approximately 5 M water (in CH(3)CN or CH(3)OH), with no reaction observed in the absence of a hydroxylic solvent, demonstrating the sensitivity of this type of ESIPT to solvent composition.  相似文献   

18.
Thiophene synthesis from furan and H2S over acid catalysts is reported. Proton donor catalysts are low-active, nonselective, and prone to deactivation. Alumina-supported catalysts having Lewis acid sites, such as alumina-supported catalysts, are more efficient. With these catalysts, the thiophene formation rate per Lewis acid site increases with increasing site strength. It is assumed that the reaction proceeds via the formation of a surface intermediate consisting of an acid site bonded to an α carbon atom of the furan ring and an H2S molecule nondissociatively adsorbed on a basic site. At atmospheric pressure, T = 250–450°C, initial furan concentrations of 1–20 vol %, and H2S/furan = 0.4–20 (mol/mol), the thiophene formation reaction is first-order with respect to both reactants and its rate constant increases with increasing temperature. The thiophene formation rate depends on the H2S/furan molar ratio. Under optimal conditions, the thiophene yield is 95–98 mol % and the thiophene formation rate is high.  相似文献   

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