聚合物异核交叉弛豫及二维NOE谱

Kover和Batta首次采用选择性质子π脉冲来测定~(13)C自旋-晶格弛豫速率并与常规反转回复法测定的自旋-晶格弛豫速率相比较求出了交叉弛豫速率,并以此来计算异核间的距离,但他们的计算方法仅适用于满足极端窄化条件的刚性球状分子。二维异核NOE谱(HOESY)是1983年才发展起来的二维NMR技术,它可用来研究异核间的交叉弛豫作用及研究分子间相互作用。Kover和Batta在此方面作了许多     

聚甲基丙烯酸正丁酯的核磁共振异核相关二维谱

<正> 核磁共振二维谱是研究高聚物分子结构的有力工具.有时一张谱图,就能得到高聚物序列结构或共聚物构型的直接证据.对高聚物结构分析有重要意义.自1983年Brown首次报道聚氯乙烯的二维J谱以来.美国Macromolecules等杂志竟相报道各种聚合物的二维谱图.目前已经报道过的聚合物核磁共振二维谱有二维J谱、~(19)F-~1H异核相关谱、~(13)C-~1H异核相关谱、~1H COSY谱、~(19)F COSY谱、NOESY     

有机磷化合物的NMR研究——Ⅲ.不对称取代1,3,2-二氮磷杂环戊烷的~(13)C NMR

本文报道了十个不对称取代1,3,2-二氮磷杂环戊烷的~(13)C 核磁共振谱,利用~(13)C 自旋-晶格弛豫时间确定了用其它去偶技术难以确定的信号的归属,讨论了偶合常数与构象的关系。     

用模型拟合法研究1,2-聚丁二烯分子运动

本文采用Cole-Cole,Fuoss-Kirkwood经验相关时间分布模型和构象跳跃,高聚物局部主链运动阻尼取向扩散分子模型,对1,2-聚丁二烯在溶液中的~(13)C-NMR自旋-晶格弛豫时间nT_1和核Overhauser效应(NOE)值进行了数值拟合。用拟合所得分子运动参数讨论了1,2-聚丁二烯微观分子运动对链结构和温度的依赖性。     

六氟磷酸二(2,2'-联吡啶)·(4,4'-二甲基-2,2'-联吡啶) 合钌(Ⅱ)的二维核磁共振谱分析

用一维NMR方法研究了电化学发光物质六氟磷酸二(2,2'-联吡啶)·(4,4'-二甲基-2,2'-联吡啶)合钌(Ⅱ)的立体结构,借助二维1H-1H COSY和1H-13C COSY实验技术对其氢谱和碳谱进行了完全的归属,并给出了其氢谱和碳谱的化学位移值.     

二羟基丙基芴基聚合物合成及光电性能研究北大核心CSCD

通过Pd催化的Suzuki聚合反应制备了侧链上含有缩酮基团的芴基聚合物PFketal,对聚合物的酸性处理得到具有羟基基团的聚合物PFOH。通过FT-IR、1 H-NMR、凝胶渗透色谱(GPC)、紫外-可见吸收光谱(UV-Vis)、光致发光光谱(PL)和循环伏安(CV)测试对聚合物进行了表征。两种聚合物具有相似的光学性质,二者在薄膜状态下UV-Vis吸收峰位于387nm处,PL发射峰值为424nm。CV测试表明PFOH相对PFketal具有较低的起始氧化电位。羟基的引入可改善聚合物在极性溶剂中的溶解度,PFOH在PFketal的不良溶剂,如二甲基甲酰胺(DMF)和二甲基亚砜(DMSO)中均具有良好的溶解度。     

六氟磷酸二(4,4'-二甲基-2,2'-联吡啶)·(2,2'-联吡啶-4,4'-二羧酸)合钌(Ⅱ)的二维核磁共振

用1H NMR和13C NMR谱研究了新型电化学发光探针六氟磷酸二(4,4'-二甲基-2,2'-联吡啶)·(4,4'-二羧酸-2,2'-联吡啶)合钌(Ⅱ)的立体结构,通过1H-1H COSY、13C-1H HETCOR谱对其氢谱和碳谱中的各谱峰进行了归属,并给出了氢谱和碳谱峰的化学位移值.     

刚性1,4-二(4-甲基咪唑)苯配体构筑的两个d10配位聚合物的合成、结构及荧光性质

利用过渡金属镉（锌）盐与1,4-二（4-甲基咪唑）苯、间苯二甲酸分别采用分层和水热法合成了化合物{[Cd（BMIB）（H₂O）₂]（NO₃）₂}_n（1）和{[Zn₂（BMIB）_1.5（OH）（IP）_1.5]·H₂O}_n（2）（BMIB=1,4-二（4-甲基咪唑）苯,IP²-=间苯二甲酸根）,并对其进行了元素分析、IR及X射线衍射法表征。晶体结构研究表明：配合物1属于三斜晶系,P1空间群。晶胞参数：a=0.382 08（3）nm,b=0.904 72（7）nm,c=1.378 29（10）nm,α=98.581（4）°,β=97.020（3）°,γ=94.398（3）°。配合物2属于单斜晶系,C2/c空间群。晶胞参数：a=3.764 07（9）nm,b=1.017 18（5）nm,c=2.015 31（11）nm,β=120.860（2）°。配合物1是由配体BMIB连接镉离子形成一维链状结构,由氢键连接成二维层结构。而配合物2是由配体IP^2-连接锌离子形成一维梯状结构,该一维梯通过羟基和BMIB连接成三维网络结构。此外,配合物1和2具有较好的荧光性能。     

两个二维层状4-双(咪唑基-1-甲基)-苯钴和镍配位聚合物的合成与表征

以1,4-双(咪唑基-1-甲基)-苯(bix)为配体,间苯二甲酸(IPA)为辅助配体,合成制备了两种新型同构配位聚合物:{[Ni(bix)(IPA)(H_2O)]}_n(1)和{[Co(bix)(IPA)(H_2O)]}_n(2)。单晶结构表明,此两个配合物均形成二维层状空间结构,金属原子均为六配位八面体结构,赤道平面上四个配位原子来自间苯二甲酸和配位水分子,轴向两个配位原子为bix配体的咪唑环上的N原子。金属原子通过配体连接形成四连接的二维4(4).6(2)方格层状结构。     

八元瓜环与二(2-亚甲基-1,2,3,4-四氢异喹啉)的自组装模式

以用1,2,3,4-四氢喹啉和二溴乙烷合成的二(2-亚甲基-1,2,3,4-四氢异喹啉)的溴化氢酸盐为客体, 八元瓜环为主体, 利用1H NMR技术, 单晶X射线衍射方法以及理论计算等方法, 考察了两者的自组装模式. 1H NMR分析结果表明, 在溶液状态条件下, 不仅每一个八元瓜环分子同时与两个客体分子的芳环部分相互作用, 而且每一个客体分子两端的芳环部分同时与两个八元瓜环分子相互作用, 从而形成一维的自组装超分子链; 而在固体状态下, 每一个八元瓜环也可同时包结两个客体的芳环部分而形成三元的自组装结构, 但八元瓜环包结两个客体形成一独立的三元自组装结构. 利用晶体结构建立模型的计算结果说明, 模拟溶液状态比固体状态条件下的主客体包结更有利于体系能量的降低, 与主客体在溶液中1H NMR实验结果相符.     

停止-流动分光光度法研究铕(II)与二甲酚橙快速电子转移反应动力学

用停止-流动分光光度法研究了Eu~(2+)与二甲酚橙(XO)间快速电子转移反应的动力学规律。求得了速控步骤的动力学参数。如反应级数(n=2)、几个不同温度下的速率常数(k_(278 K)=5.7×10~8 L·mol~-·s~(-1), k_(s38 K)=1.01×10~9 L·mol~(-1)·s~(-1))、活化能(E=7.6×10~3 J·mol~(-1)), 以及指前因子(A=1.5×10~(10) L·mol~(-1)·s~(-1)), 并判断出其为溶液中扩散控制型反应。根据实验现象与测试结果, 提出了Eu~(2+)与XO的反应分别在Eu~(2+)相对过量和在XO过量时的反应机理, 并判断了各反应步骤速率常数之间的相对关系。     

Eu(DBM)3纳米微晶的低频喇曼光谱

The fractal property and low frequency Raman scattering of Eu(DBM)3 nanosized microcrystals were investigated. The influence of the fractal structure of Eu(DBM)3 non-crystalline solids on low frequency scattering was studied. It was found that vibrational excitations on the fractal are localized and can be described in terms of fractions. It was shown that reduced Raman scattering intensity is of a power law dependence of the vibrational frequencies for all samples. The fractal and spectral dimension were also determined, we found that our experimental value was in fair agreement with the theoretical one.     

丙酮肟与某些芳烃相互作用的1H核磁共振研究

~1H NMR spectra of acetoxime have been measured as a function of the mole fraction of certain aromatic hydrocarbons in mixed solvent of CCl_4 and benzene or toluene. It has been found that the chemical shifts of the two methyl groups in acetoxime and of benzene or toluene move upfield gradually in the mixed solvent as the mole fraction of aromatic component increases. The moving rate of the resonance absorption line of the two methyl groups in acetoxime are different. The △δ of β-CH_3 is larger than that of α-CH_3. The absorption line of the two methyl groups is a singlet in CCl_4 and splits to a doublet when the concentration of benzene or toluene in the solvent is higher than 30% (mole/mole). The experimental results also show that the extent of upfield shifts of either the methyl groups in acetoxime or the aromatic hydrogens are reduced when a hydrogen of benzene is substituted by methyl group. All of the chemical shifts can be correlated with a linear equation as δ=A+Bx, Where, x is the mole fraction of benzene or toluene in the mixed solvent. The correlation coefficients R are approximately equal to -1.     

包含聚苯胺的相变材料纳胶囊的制备及其性能

采用自由基乳液聚合法和原位聚合法制备了包含聚苯胺均匀分散在正十八烷中的悬浮体系的交联聚甲基丙烯酸甲酯为囊壁的相变材料纳胶囊(NanoPCMs). 采用扫描电子显微镜(SEM)、差示扫描量热仪(DSC)、热重分析仪(TG)和广角X射线衍射仪(WAXD)等手段分别考察了成核剂聚苯胺的添加量对相变材料纳胶囊表面形态、结晶性能、热稳定性及结晶行为等的影响. 实验结果表明：包含有聚苯胺的相变材料纳胶囊,成核剂的存在对其形貌、粒径、包覆率和结晶行为影响较小,耐热性略有所降低,添加1.5 g 苯胺时生成的成核剂聚苯胺可以有效改善其过冷结晶行为.     

NH0-1+2-3离解能等的高级ab initio计算与评价

A recent experimental determination[1] of the dissociation energies (D0) for H2N-H, H2N+-H and H2N-H+, the ionization energies for NH3 and NH2 resulted in large deviations when compared with those of the earlier values and the QCISD(T)/6-311+G(3df,2p) ab initio calculations. We have performed some higher level ab initio calculations on these data by utilizing the Gaussian 92/DFT and Gaussian 94 pakages of programs and have assessed the available experimental values. Our calculations were carried out at the QCISD (TQ)/aug-cc-pVDZ, G2(QCI), QCISD(T)/6-311 ++G(3df,3pd) and QCISD(T)/aug-cc-pVTZ levels of theory. Geometries were optimized at both of the MP2(full)/6-31G(d) and the MP2(full)/6-31(d,p) levels, and were compared with those of the experiments if available. The MP2(full)/6-31G(d,p) tight-optimized geometries for the neutrals are closer to those of the experiments than those of the MP2 (full)/6-31G(d), and are in excellent agreement with the experimental results as shown in Table 1. In this case, we assumed that the optimized geometries for the cations would be better if p polarization functions are added to the hydrogen atoms. We firstly noted that the symmetry of the NH3+ cation was D3h, other than Cs. as reported in ref.[1]. All of the zero-point energies and the final geometries are calculated at the MP2(full)/6-31G(d,p) level of theory. We have also repeated the QCISD(T )/6-311 + G(3df,2p) calculations of ref. [1], because we could not identify their level of goemetry optimization. It is found that the total energy, -55.244 19 Hartrees, for NH2+(1A1 ) in ref.[1] might be in error. Our result is -55.336 29 Hartrees at the same level of theory. At our highest level [QCISD(T)/aug-cc-pVTZ] of calculations as shown in Table 3, the D0 (temperature at zero Kelvin) values of H2N-H, H2N+-H(3B1for NH2+ ) and H2N- H+ are 4.51, 5.49 and 8.00 eV, respectively. These data reported in re f.[1] were 4.97, 5.59 and 8.41 eV, respectively. Our result on D0(H2N-H) supports the work of ref.[2,3,5,6]. The ionization energies (IE) for NH3 and NH2 (3B1 for NH2+) at our highest level are 10.11 and 11.09 eV while in ref.[1] were 10.16 and 10.78 eV, respectively. For the latter, our result supports the experiment of ref.[3]. Our predicted D0 for HN2+-H and IE for NH2 (1A1 for each NH2+) are 6.80 and 12.39 eV, respectively. These values differ greatly from the predicted values (9.29 and 14.88 eV) of ref.[1] where the total energy of NH2+(1A1) might be in error. The D0 value for HN-H has not been found in ref.[1]. Our result supports the work of ref.[3]. We have also derived all of these values at the temperature of 298K and under the pressure of 101kPa at several levels of thoery as shown in Table 3. On examining the experiment of ref.[1] in detail, it is easy to find that all of the larger deviations might be from a too high value of the appearance potential of proton AP(H+). Indeed, ref.[1] has mentioned that the determintion of AP(H+), due to kinetic shift, would lead to a hihger value for the dissociation energy as has been pointed out by Berkowitz and Ruscic. In this work, we concluded that, besides some mistakes in the theoretical calculations of ref.[1], the dissociation energies for H2N-H and H2N-H+,the IE for NH2 (3B1 for NH2+) might also be unreliable and need to be re-examined.
     

黄曲霉素B1在银团簇表面吸附的表面增强拉曼光谱

采用密度泛函理论(DFT)的B3LYP方法和6-311g(d, p)(C, H, O)/LanL2DZ(Ag)基组, 优化得到黄曲霉素分子AFB₁与Ag小团簇形成的复合物AFB₁-Ag_n (n=2, 4, 6)的稳定结构, 并计算了三种复合物的表面增强拉曼光谱(SERS)和预共振拉曼光谱(SERRS), 与实验结果相一致. 计算结果显示: 三种复合物表面增强拉曼光谱中C＝O伸缩振动模的增强因子约为10²-10³, 是由于极化率改变引起的静化学增强. 根据含时密度泛函理论(TDDFT)方法计算得到的吸收光谱, 分别选择407.5、446.2和411.2 nm作为入射光, 计算三种复合物的共振拉曼光谱, 发现在SERRS光谱中, Ag―O伸缩振动的增强因子达到10⁴量级, 主要是由电荷转移产生的共振增强引起的.     

内嵌复合物X@C60中相互作用的变化规律与键本质

系统地研究了内嵌复合物Ｘ＠Ｃ６０（Ｘ＝第ＩＡ簇或第ＶＩＩＡ族元素）形成过程的能量变化,以及其中笼环境下Ｘ与Ｃ６０间相互作用的变化特征与键本质。结果表明：（１）Ｃ６０笼环境力场具有球对称性;（２）各种分解与总相互作用与内嵌原子的原子序数或原子半径呈现出规则的递变规律;（３）除Ｉ外,其余元素原子与Ｃ６０间的作用对各自复合物的稳定性都有正效应的较大贡献;（４）Ｘ在Ｃ６０笼环境中居心或偏心的稳定位置是各种     

CH(A2Δ)被O2,CS2和环乙烷猝灭的速度常数

We present the measurements of quenching rate constants of CH(A~2△) radical by O_2, cyclo-C_6H_(12) and CS_2 molecules. The time-resolved spectra of emission CH(A~2△-X~2Π) was monitored. The measured quenching rate constants are as follows. k_q(O_2)=(2.8±0.5)×10~(-11) cm~3·molec~(-1)·s~(-1)k_q(cyclo-C_6H_(12))=(2.7±0.4)×10~(-10) cm~3·molec~(-1)·s~(-1)k_q(CS_2)=(4.0±0.6)×10~(-10) cm~3·molec~(-1)·s~(-1) The value of k_q(O_2) is in good agreement with previous works. The rate constants for quenching by cyclo-C_6H_(12) and CS_2 are reported for the first time.     

C2H3自由基与O2反应的红外发射光谱及反应通道

The reaction of vinyl radicals with oxygen was investigated by Time-Resolved Fourier Transform infrared emission spectroscopy. The radicals were produced by the pulsed laser photolysis of C_2H_3Br at 248 nm. Vibrationally excited products of H_2CO(v1), HCO(v3), CO_2(v3, v), CH_3(v3), C_2H_2(v3), HO_2(v1), C_2H_2O_2(v3+v11), CO(v) formed in the C2H3+O_2 reaction have been observed. Four elementary reaction channels have been verified.