吩噻嗪-1,4萘醌-乙二醇体系光化学过程的时间分辨ESR研究

用时间分辨ESR方法研究了吩噻嗪(PTH)-1,4-萘醌(NQ)-乙二醇(RH)体系中的光化学过程.只观察到萘醌的中性半醌自由基NQH^*的全发射极化的CIDEP(化学诱导动态极化)信号,并未观察到极化的萘醌负离子NQ·^-*的CIDEP信号,表明RH与三重态NQ间的质子转移反应远比PTH与NQ间的电子转移反应为快.NQH·^*的CIDEP信号随pH值的变化表明体系中同时有极化自由基NQH·^*与NQH·₂^+*存在,并且其间有质子交换.     

TX100胶束中光解蒽醌的TRESR研究

用时间分辨电子自旋共振（ＴＲＥＳＲ） 波谱仪研究了光解蒽醌自由基的化学诱导动态电子极化（ＣＩＤＥＰ） ．实验测量表明,在蒽醌／ 乙二醇／ＴＸ－ １００ 体系中,蒽半醌自由基ＡＱＨ·有很强极化ＥＳＲ 信号,在激光激发后～０ ．８μｓ,检测到蒽醌负离子基ＡＱ·－ 的信号,表明ＡＱＨ·自由基部分地离解为负离子基ＡＱ·－ ．     

硫化镉胶粒界面自由基反应动力学的ESR研究

用电子自旋共振波谱方法研究了半导体超微粒子表面光诱导电子转移所引发的底物的次级自由基反应动力学过程.结果表明,用含有水溶性草酸盐的硫化镉(CdS)胶体体系产生的COO·^-离子基,可以较方便地引发其它自由基反应,并根据已知的由DMPO捕捉COO·^-的反应速度常数数据,去计算COO·^-基与其它可产生稳定自由基的化合物进行反应的速度常数值,从而在此基础上发展了一种研究自由基反应动力学的行之有效的简便的新途径和新方法,可以较广泛地应用于其它凝聚相的自由基反应动力学体系的研究.     

光解对苯醌/甲酰胺体系的CIDEP实验研究

以对苯醌为光敏剂,用高时间分辨电子自旋共振(TRESR)波谱仪研究了对苯醌/甲酰胺体系在酸性、碱性、胶束环境下的化学诱导动态电子自旋极化(CIDEP).光解对苯醌/甲酰胺体系,得到了以苯醌负离子基PBQ·-为主的,同时伴随稍弱的苯半醌自由基PBQH·-的发射CIDEP谱;光解碱性环境和胶束环境下的对苯醌/甲酰胺体系,只得到PBQ·-的CIDEP信号;光解酸性环境下的对苯醌/甲酰胺体系,只得到PBQH·的CIDEP信号.实验结果表明对苯醌负离子基PBQ·-由苯半醌自由基PBQ·解离得到.     

现代物理信息

 1.首次测量Ω^-的磁矩.用极化中性束的自旋转移反应产生了24700个Ω^-.     

甲基紫精与醇类间的光诱导电子转移及光催化反应的ESR研究

用ESR方法研究了甲基紫精(MV⁺⁺)与甲醇,乙醇及苄醇等之间的光诱导电子转移和光反应过程.结果发现,甲基紫精存在条件下,某些很稳定的醇类也可以发生光催化分解和光催化氧化的反应,甲基紫精在反应过程中起的是催化剂的作用在无氧条件下,MV⁺⁺/C₂H₅OH体系经UV光照10min后即可观察到很强的MV⁺离子基的信号,表明甲基紫精与乙醇分子之间发生了电子转移;当进行较长时间光辐照,则MV⁺离子基逐步消失而生成H原子和碳中心自由基。在通氧条件下进行光照时,则无MV⁺基信号而产生OOH基和碳中心自由基的信号.当体系中有一定量的水存在时,OOH基减弱而产生·OH基,且随着水量的增加,·OOH基的强度更为减弱直至消失,而同时羟基浓度则大大增加.另一个有趣而重要的现象是,对于MV⁺⁺/苄醇体系,在通氧条件下辐照时可给出很强的超氧阴离子基O₂^-的信号,而MV⁺⁺/甲醇体系可产生较弱的O₂^-信号.但是在无氧时甲基紫精的存在进行光辐照甲醇并不发生反应,而苄醇却可被甲基紫精光催化分解产生很强的苄氧基,羟甲基等自由基.本文详细地研究和讨论了甲基紫精与几种醇之间的光诱导电子转移和相应的均相光催化反应过程的机理.     

用Na2O2-DMSO体系产生O2·的ESR研究

提出了Na₂O₂的二甲基亚砜(DMsO)/H₂O溶液中产生超氧阴离子自由基(O₂^·)的新方法,用电子自旋共振仪(ESR)可直接检测到很强的O₂^·信号,研究了反应的条件及其O₂^·信号的特性,并用该法考察了茶多酚等清除剂对于超氧阴离子自由基的清除作用。结果表明本体系是产生O₂^·的有效方法,可用于超氧阴离子自由基清除剂的研究。     

吩噻嗪-1,4萘醌-乙二醇体系光化学过程的时间分辨ESR研究

用时间分辨ＥＳＲ方法研究了吩噻嗪（ＰＴＨ）－１，４－萘醌（ＮＱ）－乙二醇（ＲＨ）体系中的光化学过程．只观察到萘醌的中性半醌自由基ＮＱＨ．＊的全发射极化的ＣＩＤＥＰ（化学诱导动态极化）信号，并未观察到极化的萘醌负离子ＮＱ－·＊的ＣＩＤＥＰ信号，表明ＲＨ与三重态ＮＱ间的质子转移反应远比ＰＴＨ与ＮＱ间的电子转移反应为快．ＮＱＨ．＊的ＣＩＤＥＰ信号随ｐＨ值的变化表明体系中同时有极化自由基ＮＱＨ．＊与ＮＱＨ．＋＊２存在，并且其间有质子交换．     

丙酮/1,2-丙二醇体系的化学诱导动态电子自旋极化研究

285 nm紫外激光照射下,用时间分辨电子自旋共振(TRESR)波谱仪研究了光解丙酮/1,2-丙二醇(ACETONE/PG)体系,得到了丙酮羰自由基(CH3)2.COH和1,2-丙二醇羰自由基CH3.COHCHOH的发射/吸收(E/A)型极化信号,这是一个自由基对(RPM)极化过程。在酸性环境中,溶剂分子的CIDEP谱明显减弱,(CH3)2.COH的CIDEP谱无明显变化,由此可判断光解ACETONE/PG体系是一个夺氢反应;在碱性环境中,(CH3)2.COH反应生成负离子基(CH3)2.CO-.     

P原子的光学模型势与核极化修正

基于SIC-X_α的较为严格的计算方法,对于Rydberg电子态的交换参数采用自洽场模型计算核极化,结果比文献[15[的计算方法要精确.另外文献[15]在计算P²³⁸U的能级跃迁时,模型还不够完善,存在着难以克服的弊端,计算结果也不可能准确.20世纪70年代初,Batty就进行强相互作用势模型的研究,经过二十几次不断探索与改进,在1997—2000年给出了光学模型势的正确形式.对Rydberg电子态的交换参数采用自洽场模型计算核极化,用以修正Batty光学模型势下的P²³⁸U能级跃迁,得到反质子原子的相应能级.结果与实验数据相当符合.连同π^-,K^-,∑^-,Ξ^-原子的情况支持了Batty光学模型势在描写核子间强相互作用的正确性,同时也表明计算核极化的方法是正确的,为反粒子原子及奇特原子的深入研究及应用提供了理论依据.     

ON THE REACTION MECHANISM AND THE SELECTION RULE IN THE DOUBLE CHARGE EXCHANGE REACTION OF PIONS ON NUCLEI (DCX)-A STUDY OF THE CONNECTION BETWEEN THE 2β-DECAY AND DCX ON jP=O+ NUCLEI

It is shown that in the pion induced double charge exchange reaction on J^p=O⁺→O⁺ nuclei,there exists a possible new reaction mechanism π⁺(Δ⁰,Δ⁺⁺)π^- or π⁺(Δ^-,Δ⁺)π^- in so-called single step process,while that old speculative mechanism π⁺(N,Δ)π^- or π⁺(N,Δ)π^- is firbidden by a well-known selection rule which has been indicated in the theory of the nuclear 2β-decay.     

ANALYSIS OF SOME HYPERCHARGE EXCHANGE REACTIONS OF THE TYPE 0-+1+/2→2++1+/2 at 4 GeV/c

The differential and integrated cross section data for the hypercharge exchange reactions ^πp→K°(1420)Λ, K ^- p→f°Λ and K ^- p→f^′Λ at 4 GeV/c are fitted by using as imple Regge pole model with phenorncnological residue functions. It is assumed that each of the two non-degenerate K^* and K^** trajectories, exchanged in this reaction, is coupled only to one of the two independent helicity amplitudes.     

菁染料光敏化超氧自由基的产生

本文用自旋捕捉技术研究了青染料在含氧的二甲基亚用溶液中将氧光还原成超氧自由基的反应,在水溶液中光照时产生的羟基自由基来源于是初形成的O₂^·。超氧负离子的形成是由于电子从激发态染料转移至溶解的氧,各种染料的光致ESR信号强度与染料的氧化还原电位有关。     

STUDIES OF P-MESCN DECAY BY THE TRANSITION POTENTIAL Vq-qqq OF A QUARK-ANTIQUARK PAIR CREATIOR MODEL

Decay rate of p-meson into two n-mesons was calculated by using the transition potential of a quark-antiguark pair creation model.The theoretical result is in good agreement with the experimental data .Also, the difference of decay widths for processes ρ^±π^±π⁰ and ρ⁰π⁺π^- was discussed.     

Vacuum Polarization Bubble Effects on the Triangle Relations for B Meson Charmless Decay Amplitudes

Assuming that factorization is valid and that contributions of the exchange, annihilation, and penguin-annihilation diagrams are negligible, we study the effects of the QCD vacuum polarization bubbles on the decay amplitudes of some B meson charmless decays into two light pseudoscalars. The bubbles have much less effects on B⁰→π⁺π^-, π^-K⁺, π⁰K⁰ than on B⁰→π⁰π⁰ thus the triangle relation √2A(B⁺→π⁺π⁰) = A(B⁰→π^-K⁺)/R_u+√2A(B⁰→π⁰K⁰)/R_u is changed slightly while √2A(B⁺→π⁺π⁰)=√2A(B⁰→π⁰π⁰)+A(B⁰→π⁺π^-) is altered significantly. This may indicate that in order to test or use these triangle relations other higher order QCD corrections should also be carefully taken into consideration.     

THE SYMMETRIC STRUCTURE OF EXCITED STATES OF 13ΛC AND INVESTIGATIONS OF THE ANGULAR DISTRIBUTIONS OF 13C(K-,π-)13ΛC*

Based on the meth SU₃ × SU₂ supermultiplet classification,we studied the symmetric compon-ents of 10.4 and 16.4 MeV configuration of the ¹³_ΛC hypernucleus by calculating the hypernucleus by calculating the angular distribution of ¹³C(K^-,π^-)¹³_ΛC^* in the framework of DWIA, and analysed the effects of varying the parameters on the angular distributions.     

THE π-NUCLEUS INELASTIC SCATTERING AND THE NUCLEAR CORE EXCITATION FOR 13C

Using the DWIA with eikondl distorted waves and by considering nuclear core excitation, we we calculate the differential cross section of the inelastic scattering for the excitation of the 3/2^- (3.68 Mev) and the 5/2^- (7.55 Mev) states in ¹³C at T_π =180 Mev. Our results agree well with the expetiments data.     

Two Higgs Doublet Model III and Double-Lepton Polarization Asymmetries in ∧b→∧μ+μ- Decays

Using the form factors calculated both in lattice QCD and HQET, we analyze the branching ratio, double- lepton polarization asymmetries and averaged double-lepton polarization asymmetries of ∧_b→∧μ⁺μ^- decay in the 2HDM III, respectively. Combining the experimental constrains on the 2HDM III parameters, we take two set of representative parameter spaces in our calculations. For the branching ratio of ∧_b→∧μ⁺μ^- decay, considering the uncertainties of the form factors and input parameters, we find the results of both SM and 2HDM III can satisfy the current experimental data in the framework of lattice QCD, but not in HQET. Then we calculate the double-lepton polarization asymmetries P_ij and their averaged values ij>, we find the double-lepton polarization asymmetries P_LT, P_NN, and P_TT are sensitive to the 2HDM III. However, P_LN, P_NL, P_NT, and P_TN show the opposite results. The contribution of the 2HDM III to their averaged values have similar results.     

Low-lying electronic states of CuN calculated by MRCI method

The high accuracy ab initio calculation method of multi-reference configuration interaction(MRCI) is used to compute the low-lying eight electronic states of CuN.The potential energy curves(PECs) of the X~3∑~-,1~3Π,2~3∑~-,1~3△,1~1△,1~1∑~-,1~1Π,and ~5∑~- in a range of R=0.1 nm-0.5 nm are obtained and they are goodly asymptotes to the Cu(~2S_g) + N(~4S_u) and Cu(~2S_g)+N(~2D_u) dissociation limits.All the possible vibrational levels,rotational constants,and spectral constants for the six bound states of X~3∑~-,1~3Π,2~3∑~-,1~1△,1~1∑~-,and 1~1 Π are obtained by solving the radial Schrdinger equation of nuclear motion with the Le Roy provided Level 8.0 program.Also the transition dipole moments from the ground state X~3∑~- to the excited states 1~3Π and 2~3∑~- are calculated and the result indicates that the 2~3∑-X~3∑ transition has a much higher transition dipole moment than the 1~3Π-X~3∑~- transition even though the l~3Π state is much lower in energy than the 2~3∑~- state.