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1.
从番麻(Agave americana L.)发酵的叶汁中分离得到红光皂甙元(hongguanggenin)、Cantalasaponin-1及一个新的甾体皂苷Agameroside-1. 运用2D NMR技术,包括DQF 1H-1H COS Y,HSQC,HMBC,HSQC-TOCSY,ROESY等技术,首次全归属了3个甾体化合物的氢和碳的化学位移,并总结了红光皂甙元的甙化位移效应,从而修正了文献中部分碳信号归属以及甙元的甙化位移效应.  相似文献   

2.
韩秀文  于海 《波谱学杂志》1999,16(6):533-540
用同核和异核二维核磁共振方法全归属了一系列合成的薯蓣皂甙元-β-D葡萄糖甙的1H和13C核磁共振谱线.这些薯蓣葡萄糖甙是薯蓣皂甙元-β-D葡萄糖甙(1),薯蓣皂甙元-β-D葡萄糖基-(1→2)-β-D葡萄糖甙(2),薯蓣皂甙元,-β-D葡萄糖基-(1→3)-β-D葡萄糖甙(3),薯蓣皂甙元[-β-D葡萄糖基-(1→2)-β-D葡萄糖基(1→3)-β-D葡萄糖甙(4)以及薯蓣皂甙无[-α-L鼠李糖基-(1→2)]-β-D葡萄糖基-(1→3)-β-D葡萄糖甙(5).  相似文献   

3.
用同核和异核二维核磁共振方法全归属了一系列合成的薯蓣皂甙元-α-鼠李糖基-β-D葡萄糖甙的1H和13C核磁共振谱线.这些薯蓣葡萄糖甙是薯蓣皂甙元-β-D葡萄糖甙(1),薯蓣皂甙元-α-L鼠李糖基(1→2)-β-D葡萄糖甙(2),薯蓣皂甙元-α-L鼠李糖基(1→4)-β-D葡萄糖甙(3),薯蓣皂甙元[-α-鼠李糖基-(→2)]-α-L鼠李糖基→-(1→4)-β-D葡萄糖甙(4)以及薯蓣皂甙元[-α-L鼠李糖基-(1→2)]-β-D阿拉伯糖基-(1→4)-β-D葡萄糖甙(5).  相似文献   

4.
二维核磁共振波谱归属人参二醇的NMR谱线   总被引:6,自引:0,他引:6  
人参二醇是构成人参皂甙的三种甙元之一,具有较高的生物活性,对它的生理活性和药理作用研究证明:人参二醇具有一定的抗肿瘤作用,本文报道用异核COSY、COLOC-S等2D NMR方法归属人参二醇的13C和1H化学位移.  相似文献   

5.
20(R)和20(S)-人参皂甙Rg2碳氢NMR信号全指定   总被引:10,自引:2,他引:8  
20(R)和20(S)人参皂甙Rg2属于达玛烷型四环三萜类化合物.应用2DNMR技术:1H-1H COSY、HMQC和HMBC全归属20(R)和20(S)人参皂甙Rg2碳和氢质子信号,为该类型化合物的结构鉴定提供波谱学依据.  相似文献   

6.
用同核和异核二维核磁共振方法全归属了一系列合成的薯蓣皂甙元-β-D葡萄糖甙的1H和13C核磁共振谱线.这些薯蓣葡萄糖甙是薯蓣皂甙元-β-D葡萄糖甙(1),薯蓣皂甙元-β-D葡萄糖基-(1→2)-β-D葡萄糖甙(2),薯蓣皂甙元,-β-D葡萄糖基-(1→3)-β-D葡萄糖甙(3),薯蓣皂甙元[-β-D葡萄糖基-(1→2)-β-D葡萄糖基(1→3)-β-D葡萄糖甙(4)以及薯蓣皂甙无[-α-L鼠李糖基-(1→2)]-β-D葡萄糖基-(1→3)-β-D葡萄糖甙(5).  相似文献   

7.
二维接力-HOHAHA和NOE差谱法测定甙类化合物的结构   总被引:1,自引:0,他引:1  
该文提出一种新的二维接力-HOHAHA实验方法.研究结果表明,该方法可用于从高度重迭的谱图中分离出各个糖体的1H NMR信号,并且与NOE差谱实验相结合可以用于测定甙类化合物中糖体间和糖体与甙元间的连接位置.本方法以1H NMR为基础,故其灵敏度比以13C NMR为基础的甙化位移方法高得多.  相似文献   

8.
黄酮类化合物-O-甙的13C NMR谱   总被引:1,自引:0,他引:1  
概述了黄酮类化合物-O-甙(包括双糖甙及寡糖甙)的13C NMR谱鉴定中涉及的溶剂选择,糖的数目与鉴定,糖的端基信号与甙化位移,甙元的鉴定,双糖及寡糖甙中各单糖的连接次序,以及糖链上的酰基取代等.  相似文献   

9.
运用2D NMR技术,如DQF 1H-1H COSY,HMQC,HMBC,TOCSY等,对3 个原人参二醇型双糖链配糖体人参皂甙-Rd,三七皂甙-E和七叶胆皂甙XVII的氢和碳的化学位移首次进行了全归属.  相似文献   

10.
用远程1H-13C COSY (HMBC)技术研究了从朝鲜淫羊藿中分离出的二个脱水淫羊藿素-3-O-甙类化合物,朝藿甙A和箭藿甙B,确定了其骨架碳的化学位移.并重新评估了前期文献对该类化合物C-5、C-7和C-4'信号的归属.  相似文献   

11.
12.
本文以aug-cc-pv5Z为基组, 采用考虑Davidson修正的多参考组态相互作用方法(MRCI+Q)得到了GeS分子基态(X1Σ+)和5个低激发态(11Σ, 11Δ, A1Π, 15Σ+, 25Σ+)的势能曲线. 计算结果表明: 25Σ+态为排斥态, 其余5个态为束缚态; 6个态有着共同的离解通道, 离解极限均为Ge(3P)+S(3P). 利用计算得到的势能曲线得了X1Σ+, 11Σ-, 11Δ, A1Π和15Σ+态的垂直跃迁能Te, 平衡键长Re, 离解能De, 谐振频率ωe, 非谐性常数ωexe及平衡位置的电偶极矩. X1Σ+态的Re 为2.034 Å, De 为5.728 eV, ωe为571.73 cm-1, ωexe为1.6816 cm-1, 平衡位置的电偶极矩为1.9593 Debye. 激发态11Σ, 11Δ, A1Π, 15Σ+的Te 依次为25904.81, 26209.22, 32601.19, 43770.26 cm-1; Re依次为2.313, 2.322, 2.188, 2.8790 Å; De依次为2.524, 2.487, 1.694, 0.3036 eV, ωe依次为358.90, 353.08, 376.32, 134.96 cm-1; ωexe依次为1.2421, 1.2151, 1.6608, 1.9095 cm-1; 平衡位置的电偶极矩依次为1.3178, 1.4719, 1.5917, -1.9785 Debye. 通过求解核运动的薛定谔方程得到了J=0时X1Σ+, 11Σ-, 11Δ, A1Π和15Σ+态前30个振动态的振动能级Gv和分子常数Bv, 得到的结果和已有的实验值及其他理论值符合较好.  相似文献   

13.
If the contacts of a vacuum interrupter open shortly before a current zero, the transient recovery voltage (TRV) can cause a reignition and reestablish the arc. When the current in a diffuse vacuum arc passes through zero, there is a distinct pause before the TRV builds up (approximately 40 ns for copper). During this pause the gap carries conduction current only with an ion component which depends on dI /dt, varying between 3 A for dI/dt=60 A/μs and 60 A for dI/dt=1235 A/μs. The ion current subsequently decays in tens or hundreds of nanoseconds. It can be distinguished from the displacement current at this time by varying dV/dt, keeping the other parameters constant. Among the interruption criteria for short high-frequency vacuum arcs, dI /dt prior to current zero and initial dV/dt are the most important. High values of dI/dt are more likely to precipitate reignitions, but breakdowns can occur after lower dI/dt's if the gap has been subjected to a high current for a relatively long time (>100 μs)  相似文献   

14.
傅里叶红外光谱研究血清白蛋白构象   总被引:5,自引:0,他引:5  
用傅里叶红外光谱法研究了BSA及其水溶液的红外光谱。通过对其酰胺I带傅里叶自转积谱分析,为其及部分水溶液中的二级结构构象进行了指认。结果表明,BSA水溶液状态与固态时的二级结构是不同的。随着溶液浓度的降低,酰胺I带二级结构峰存在明显的位移现象,即1609.86cm^-1位移到1608.24cm^-1,1633.85位移到1638.36cm^-1,1653.69cm^-1位移到1656.10cm^-  相似文献   

15.
Under GGA, the structural, electronic properties and stabilities of four different (1 × 1) terminations of cubic PbTiO3 (1 1 1) surface, the directly cleaved (1 1 1)-Ti and (1 1 1)-PbO3 terminations and the constructed (1 1 1)-TiO and (1 1 1)-PbO2 ones, have been systematically studied by using projector-augmented wave method implemented in VASP. For (1 1 1)-Ti and (1 1 1)-PbO3 terminations, Ti-O bonds between the outermost two layers are enhanced after relaxation, while those between the second and the third layers are weakened. In addition, a contraction of O-O distance in surface PbO3 layer is also found for (1 1 1)-PbO3 termination. Moreover, electronic structures of both (1 1 1)-Ti and (1 1 1)-PbO2 terminations are significantly influenced by structure relaxations, and the effects of the surface on the DOS are dominantly on the Ti layers, especially the CB. For a constructed (1 1 1)-TiO termination, the relaxation results show both Ti-O bonds between the outermost two layers and those between the second PbO3 layer and the third Ti layers are enhanced. For a constructed (1 1 1)-PbO2 termination, Ti-O bonds between the outermost two layers are also enhanced as in the (1 1 1)-TiO termination, however, inequivalent Ti-O bonds between the second layer Ti atom and the third layer O atoms are found, with two bonds expanding and the other one contracting. Results of electronic structure calculations show these two constructed terminations are all insulating and changes of DOS originate dominantly from modifications of surface compositions. Furthermore, it is found that for all four different (1 1 1) terminations, the movements of the cation and/or anion on the outermost layer along the surface normal direction after relaxation all result in a reduction of the space electric field. In O and Pb external environments, it is predicted that (1 1 1)-PbO2 termination is the most stable one in O- and Pb-rich environments, however, the (1 1 1)-Ti termination is stable one in O- and Pb-poor conditions. The (1 1 1)-TiO termination also shows a stability domain in moderate O and Pb environments.  相似文献   

16.
超快光电测量技术   总被引:3,自引:0,他引:3  
本文综述了近年来趔快光电测量技术的新进展,其中包括扭快光电材料的特性、高速光电器件的基本原理,着重介绍了若干主要的用快光电测量技术.  相似文献   

17.
应用红外光谱法鉴别肉苁蓉及其混淆品草苁蓉和锁阳   总被引:3,自引:0,他引:3  
采用傅里叶变换红外光谱法结合二维相关分析技术分别对药用植物肉苁蓉及其混淆品草苁蓉、锁阳进行了鉴别研究.结果表明,三者的红外光谱图表现出了一定的差异性:肉苁蓉在1 730和931 cm-1有吸收峰,草苁蓉在1 510,1 375,1 266 cm-1处存在吸收峰,锁阳的最高峰位于1 614cm-1处.在二阶导数谱图上三者差异更加明显:肉苁蓉在1 453,1 336,931,892 cm-1处都有较强的吸收峰.其中931 cm-1处的吸收峰较尖锐,强度也最强;草从蓉的最强峰位于1 509 cm-1,并且1 633和1 161 cm-1处的吸收峰明显变宽,强度也变大;锁阳在1 682cm-1处有较尖锐的吸收峰,1 605 cm-1附近的吸收峰强度也较大.二维红外谱图不但差别明显,而且直观.三者提取物的红外光谱同样存在显著差异.应用该方法能够实现肉苁蓉药材与混淆品的快速、准确鉴别.  相似文献   

18.
Z. Dohnálek 《Surface science》2006,600(17):3461-3471
Thin Pd films (1-10 monolayers, ML) were deposited at 35 K on a Pt(1 1 1) single crystal and on an oxygen-terminated FeO(1 1 1) monolayer supported on Pt(1 1 1). Low energy electron diffraction, Auger electron spectroscopy, and Kr and CO temperature programmed desorption techniques were used to investigate the annealing induced changes in the film surface morphology. For growth on Pt(1 1 1), the films order upon annealing to 500 K and form epitaxial Pd(1 1 1). Further annealing above 900 K results in Pd diffusion into the Pt(1 1 1) bulk and Pt-Pd alloy formation. Chemisorption of CO shows that even the first ordered monolayer of Pd on Pt(1 1 1) has adsorption properties identical to bulk Pd(1 1 1). Similar experiments conducted on FeO(1 1 1) indicate that 500 K annealing of a 10 ML thick Pd deposit also yields ordered Pd(1 1 1). In contrast, annealing of 1 and 3 ML thick Pd films did not result in formation of continuous Pd(1 1 1). We speculate that for these thinner films Pd diffuses underneath the FeO(1 1 1).  相似文献   

19.
A general theory is developed for self-consistent calculations of mode competition in a gyrotron with nonfixed axial structure of the RF field for arbitrary cyclotron harmonics. The theory is applied to the gyrotron operating at the Kernforschungszentrum Karlsruhe with a frequency of 150 GHz. The formalism presented allows a self-consistent calculation of mode competition for the operating and parasitic modes at the cyclotron resonance at arbitrary harmonics. Specific calculations are carried out for the cases n0=1, n1 =2 and n0=2, n1=1. It is emphasized that the formalism considered applies only to the case in which the azimuthal orthogonality condition is satisfied: n0m1n1 m0. There are circumstances when this condition is not satisfied  相似文献   

20.
八角茴香与其伪品莽草的红外光谱三级鉴定研究   总被引:2,自引:0,他引:2  
采用红外光谱三级鉴定的方法区分和鉴别了八角茴香及其伪品莽草。红外光谱三级鉴定即依次采用一维红外光谱、二阶导数谱和二维相关红外光谱,分辨率逐渐提高,谱图的差别也进一步放大。一维谱图中,两者整体峰形比较相似,但在3400 cm-1附近八角茴香只出现一个特征峰3392 cm-1,而莽草则出现3482和3387 cm-1两个特征峰。二阶导数谱在850~1180 cm-1波段八角茴香的几个强峰峰强相对比较接近,其中1015 cm-1为图中最强峰,而莽草的最强峰在1070 cm-1附近;在1180~1500 cm-1波段八角茴香在1469,1454,1442 cm-1附近的3个特征峰峰强明显强于1292,1276,1 266 cm-1附近的特征峰,而莽草则刚好相反。二维相关红外光谱中差异更明显,850~1165 cm-1波段八角茴香在主对角线上的自动峰较强峰出现在1153和1000 cm-1,而莽草峰强较强的自动峰出现在911和878 cm-1;1165~1500 cm-1波段八角茴香呈现2个自动峰,而莽草则出现5个自动峰。可见红外三级鉴定方法是一种快速有效的鉴定中药材的方法。  相似文献   

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