采用固体NMR研究MPEG-PLA双嵌段共聚物的固态相区结构

采用固体核磁共振方法，研究了AB型聚（L-丙氨酸）聚乙二醇嵌段共聚物(MPEG-b-PLA）的固态微相结构. ¹³C核的交叉极化与直接极化实验表明，MPEG中存在晶态和非晶态两种相区结构，PLA则含有大量的α螺旋与少量的β折叠二级结构. 由交叉极化过程下的¹³C自旋-晶格弛豫时间(T₁)测定结果进一步表明，MPEG链段由于嵌段结构使结晶过程受抑制，结晶度明显下降. PLA链段以结晶态形式存在，并由于大量α螺旋和β折叠有序结构的存在, 链段非常刚性，运动严重受限，而β位甲基因为可以自由旋转，所以运动能力较α位次甲基和羰基强.     

单取代苯的自旋-晶格弛豫时间T1和NOE增强因子η与取代基电负性能标的关系

本文对甲苯、乙基苯、硝基苯、卤代苯等单取代苯的¹³C自旋-晶格弛豫时间T₁和NOE增强因子η与取代基电负性能标的关系进行了探讨。     

固体核磁共振研究半晶聚-3-羟基丁酸酯和聚羟基丁酸戊酸酯的分子动力学

本文在150~370 K温度范围内,采用固体核磁共振（NMR）测定了半晶聚-3-羟基丁酸酯（PHB）,以及3-羟基戊酸酯单体质量分数分别为5%（PHBV5）和12%（PHBV12）的聚羟基丁酸戊酸酯共聚物在实验室坐标系和旋转坐标系条件下质子的自旋-晶格弛豫时间T₁和T_1ρ.通过弛豫时间随温度变化的理论拟合,分别获得上述半晶聚合物晶区和结晶区的分子动力学参数（包括E_a和τ₀）.这些结果从分子水平上阐述了PHB结构修饰和增强的原因.     

结晶PMMA的NMR研究

用NMR方法和DSC技术研究了结晶聚甲基丙烯酸甲酯(PMMA)性质和玻璃化转变温度,并与无定形PMMA作了比较.通过¹³C CPMAS谱,观察到了结晶PMMA与无定形PM MA的谱的线形,线宽,化学位移都十分类似,其中α-CH₃分裂为两个峰,我们将它归属为γ旁式效应所对应的反式和旁式构象.而反门控碳谱显示PMMA中有四种状态,即等规PMMA结晶态和无定形态,间规PMMA结晶态和无定形态.通过测定T₂(H)和旋转坐标系中质子的自旋晶格弛豫时间T_1ρ(H),我们分别得到了两T₂(H)值和两个T_1ρ(H)值,对应于晶区与非晶区,而且其含量分别与反门控碳谱积分所得含量一致.     

丙烯腈γ辐射聚合的NMR研究

用¹H NMR、¹³C NMR谱、自旋-晶格弛豫时间（T₁）和自旋-自旋弛豫时间（T₂）研究了丙烯腈在⁶⁰Co γ射线辐射聚合后的大分子结构变化与大分子链的运动. 结果表明随着辐射剂量增大，在单体形成聚合物的过程中，聚合物主链上出现了少量的-OH基团，继续增大辐射剂量， -OH部分被氧化. 对聚合物溶液的变温氢谱的研究表明，溶剂中的残余水与上述-OH形成氢键，且随着温度升高氢键被破坏，同时H₂O与-OH之间还存在着质子交换. 利用¹³C NMR谱对丙烯腈辐射聚合的产物进行了序列结构分析. 对T₁和T₂的研究表明，辐射剂量的增大并未影响到聚丙烯腈的链运动，证明了在丙烯腈的辐射聚合过程交联反应未发生.     

激光极化129Xe核自旋弛豫率的测量

由弱磁场下光泵自旋交换、强磁场中核磁共振测量方法,获得激光极化低压同位素¹²⁹Xe气体的核自旋弛豫率1/T₁及其与N₂气压力、环境温度的关系.结果表明:在291K的室温下,对于0~11 333.05Pa的N₂气压力范围,1/T₁随着N₂气压力的增加而增大;N₂气压力为1 466.63Pa时,1/T₁随着样品温度从234K到292K增高而减小     

未掺杂聚乙炔中质子的自旋晶格弛豫——局域化的孤子

测量了未掺杂的顺式聚乙炔(cis-polyacetylene)、反式聚乙炔(trans-polyacetylene)和部分氘代的反式聚乙炔样品的质子自旋晶格驰豫时间T₁,测量了反式聚乙炔的旋转座标系中的质子自旋晶格弛豫时间T_1ρ。结果表明,反式聚乙炔中确实存在大量被称为孤子(Soliton)的自旋中心,它们是质子弛豫的支配因素。孤子是可动的,但又是局域化的。用局域化的孤子模型,不仅说明了T_1ρ过程的多指数型衰减,也解释了它的衰减速率不随温度和自旋锁定场强度而变化的特点。     

PAMAM树状大分子与5-氟尿嘧啶相互作用的NMR研究

本文利用多种核磁共振（NMR）技术研究了聚酰胺-胺树状大分子（PAMAM）与5-氟尿嘧啶（5-FU）在水溶液中的相互作用.¹H NMR化学位移滴定结果表明5-FU分子结合在PAMAM分子表面,¹³C NMR化学位移滴定分析结果表明5-FU分子通过氢键或疏水间相互作用进入到PAMAM的内部疏水空腔.¹H核和¹⁹F核自旋-晶格弛豫时间（T₁）的测定结果也说明了二者之间存在相互作用.NOESY实验进一步验证了5-FU分子进入到PAMAM分子的内部空腔.本研究为研究树状大分子和药物小分子的相互作用提供了系统的NMR分析方法.     

苯乙烯和马来酸酐共聚物的13C NMR谱解析和分子链结构表征

通过比较高温110 ℃下特定苯乙烯-马来酸酐共聚物H10和常温紫外辐照特定共聚合的苯乙烯-马来酸酐共聚物UV4的¹³C质子去偶谱和DEPT135谱，总结给出共聚
物链中马来酸酐环中酸酐基的取代效应参数（α=13.5、β=2.5、γ=-2）及引用苯基取代参数：α=16、β=6、γ=-2，对共聚物主链碳的化学位移进行了经验计算，对所有碳，尤其是主链碳在三单元组或四单元组水平上进行了链序列结构归属. 在进行峰面积积分的基础上，对共聚物分子链两种组份摩尔比或摩尔含量、交替度、链嵌段长度、马来酸酐环残基中顺反异构体比和共聚物数均分子量等进行了表征. 共聚物UV4比H10的交替度高许多，表明聚合温度对苯乙烯和马来酸酐共聚合交替链结构的形成有重要影响.     

基于多弛豫信号补偿的快速磁共振T1ρ散布成像

定量磁共振成像（MRI）可量化组织特性,是科学研究和临床研究的重要工具.旋转坐标系下的自旋-晶格弛豫时间（T_1ρ）能反映水与大分子之间的低频交互作用,在3 T及以上的高场环境下,T_1ρ受水和不稳定质子之间化学交换的影响较大,通过测量弛豫率随自旋锁定场强度的变化而得到其分布情况（T_1ρ散布）,可用于分析和量化质子的交换过程,因此T_1ρ散布是一种重要的定量MRI技术.然而,获得不同自旋锁定场强下T_1ρ加权图像的时间过长,限制了其应用范围.针对这一问题,本研究提出一种基于多弛豫信号补偿策略的快速T_1ρ散布成像方法.该方法将不同锁定频率下的T_1ρ加权图像补偿到同一信号强度水平,并结合低秩与稀疏建立重建模型.实验结果表明,该方法在加速倍数高达7倍时仍获得了较好的重建结果.     

Effects of magic-angle spinning on spin-lattice relaxations in talc

The spin-lattice relaxation times T₁ of ¹H and ²⁹Si spins in talc have been measured at room temperature with and without magic-angle spinning (MAS) of the sample. Paramagnetic impurities work as relaxation centers. ¹H T₁ depends on the spinning rate, whereas ²⁹Si T₁ is independent of the spinning rate. These facts demonstrate that spin diffusion plays an important role in ¹H relaxation but not in ²⁹Si relaxation. ²⁹Si spins relax through dipole-dipole interactions with electron spins directly, which mechanism is not affected by spinning. The relaxation rates have been analyzed theoretically.     

Measurement of spin-lattice relaxation times of C in organic solids

A transient nuclear Overhauser effect (NOE) makes measurements of the ¹³C spin-lattice relaxation times in organic solids complicated. Extended Solomon equations are applied in order to describe ¹³C spin-lattice relaxation with ¹H r.f. field irradiation. Spin-lattice relaxation under r.f. irradiation is shown to be generally a triple-exponential process, but it can be reduced to be single-exponential under stronger r.f. field irradiation as well as in the absence of ¹H initial magnetizations. Based on numerical calculations, the difference between spin-lattice relaxation curves obeying T₁^C < T₁^H and those obeying T₁^C < T₁^H is clearly indicated. The methyl group resonances in solid-state -valine are examined, and the experimental results agree well with the theoretical results.     

丙硅乳液的核磁共振研究

单介绍了²⁹Si NMR实验技术;用²⁹Si NMR测定了丙硅乳液原料羟基硅氧烷的平均聚合度、平均分子量、平均羟基含量;用¹³C NMR分析了丙硅乳液的结构组成。     

C CPMAS studies of plant cell wall materials and model systems using proton relaxation-induced spectral editing techniques

The solid state ¹³C CPMAS NMR spectra of plant cell walls are often complex owing to superposition of resonances from different polysaccharides and the heterogeneity of the cell wall assembly. In this paper, we describe the application of a set of proton relaxation-induced spectral editing (PRISE) experiments which combine ¹H relaxation properties (T₁, T_1ρ, T₂) with ¹³C high resolution spectroscopy (CPMAS) to relate the dynamics of the plant cell walls and model systems to their domain structural details. With PRISE it has been found that in plant cell wall materials, cellulose is always associated with the long components of spin–lattice relaxation in both the laboratory and rotating frames whereas non-cellulose polysaccharides (pectin and hemicellulose) are associated with the short ones. For the proton T₂ relaxation, cellulose is only associated with the short component (below 20 μs), pectin contributes to both the short component and the long one.     

Solid-state NMR and 2,3-dicyano-5,7-dimethyl-6H-1,4-diazepine

Crystalline 2,3-dicyano-5,7-dimethyl-6H-1,4-diazepine (A) was investigated by solid-state NMR spectroscopy, X-ray diffraction, and spectral simulations. The solid-state ¹³C NMR spectra of A display peculiar splittings for the methyl and cyano resonances. The crystal structure of A indicates that the methyl doublet is a consequence of two crystallographically inequivalent environments. The methyl motions associated with each site was examined via spin-lattice relaxation time (T₁) measurements, and the carbon relaxation times (T₁^C) were used to calculate energy barriers to methyl rotation. The energy barriers to rotation were then used to correlate each methyl ¹³C shift with a particular crystallographic environment. The complex cyano splittings, however, are a result of both crystallographic inequivalence and residual ¹³C–¹⁴N dipolar coupling. The multiplet patterns of the isotropic shifts (centerbands) are dependent upon the magic-angle spinning (MAS) rate. Spectral simulations, using the perturbation method, of the centerbands and first-order sidebands were used to demonstrate, and elucidate, the observed MAS rate-dependent multiplet patterns of the cyano signals.     

Nuclear magnetic resonance relaxometry of the normal heart: Relationship between collagen content and relaxation times of the four chambers

The use of nuclear magnetic resonance (NMR) relaxation time measurements for characterization of abnormal cardiac tissue depends upon knowledge of variations of relaxation times of normal myocardium and determinants of these variations. We calculated in vitro NMR T₁ and T₂ relaxation times of canine myocardium from the four cardiac chambers, and determined hydroxyproline concentration (as a measure of collagen) and percent water content of the samples. We found both water content and T₁ relaxation time of the right ventricle to be significantly greater than the left atrium (p < 0.05). T₂ relaxation time of the left ventricle was found to be shorter than each of the other three chambers (p < 0.05). There were significant correlations between the spin-lattice relaxation time and both percent water content (r = 0.58) and hydroxyproline concentration (r = 0.45). A significant correlation was also found between T₂ relaxation time and hydroxyproline concentration (r = 0.49). When T₁ and T₂ were adjusted for water and hydroxyproline content, there was no longer any evidence for significant interchamber differences for either T₁ or T₂. These data suggest that differences in NMR relaxation times exist among the four chambers of the normal canine heart. Furthermore, a major determinant of myocardial spin-lattice relaxation time is tissue water content while both collagen content and percent water content significantly contribute to variability in cardiac chamber T₂ relaxation times.     

环二硅氨烷的29Si和13C NMR研究

本文报道了十种环二硅氨烷衍生物(R₁=Me、ф;R₂=Me、ф1 R₃=Me;X=Me、ф、OH、OSiMe₃、H和cl)及与此有关的九种聚合物m+n(m=2,3,4,7,10)的²⁹Si和¹³C化学位移,讨论了取代基X、R₁、R₂及硅氧链节数m对化学位移的影响。通过考察化学位移随R₁、R₂的变化,推断环二硅氨烷中N与其周围的三个Si之间存在(p→d)π相互作用。     

Synthesis and structural characterization of mixed aluminum-gallium-offretites

A new synthesis procedure is reported for the preparation of mixed Al,Ga-offretites over the entire solid solution range 0 ≤ Ga/(Ga + Al) ≤ 1. The resulting materials are characterized by X-ray powder diffraction, adsorption microcalorimetry and multinuclear solid state NMR. The ²⁹Si MAS-NMR data are consistent with statistical occupancy of the T₁ and T₂ sites by aluminum and gallium, and also show no positive evidence for preferential siting effects between both framework metals. Isotropic chemical shifts and nuclear electric quadrupolar coupling constants for ²⁷Al and ⁷¹Ga have been obtained from a field-dependent analysis of the center of gravity in the MAS-NMR spectra. H-Al, Ga-offretites produced by ammonium exchange and subsequent calcination reveal evidence of partial demetallation of the framework with formation of extra-lattice metal species.     

螺吲哚啉萘并噁嗪衍生物的1H、13C NMR谱法研究

本文报道了1-18烷基-3,3-二甲基螺吲哚啉萘并噁嗪及其5'-COOMe,8'-Br衍生物在氯仿和四氯化碳中的¹H和¹³C NMR结构特征。     

Correlation between 1H FID and T1rho components in heterogeneous polymer systems: an application to SBS

Wideline ¹H FID and relaxation measurements of a relatively simple motionally heterogeneous system, the triblock copolymer styrene–butadiene–styrene, have been performed in a temperature range between the polystyrene and polybutadiene glass transition temperatures. The two FID and the two spin lattice relaxation time in the rotating frame (T_1ρ) components found at each temperature have been correlated by means of a two-dimensional approach. It is shown that this approach allows dynamic information, not accessible simply by interpreting proton T₁ and T_1ρ data, to be revealed. In the case examined, the correlation found could be confirmed by high-resolution ¹H T_1ρ-selective ¹³C Cross Polarization experiments.