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IR LMR HYPERFINE RESOLVED SPECTRUM OF THE ν 3 BAND OF 14 N16 O2
LIU Xiaoyong, GUO Yuanqing, HUANG Guangming, LIN Jieli, LIU Hongping, LI Fengyan, LI Jinrui, GAO Hui, LIU Yuyan
Chinese Journal of Magnetic Resonance, 2000, 17(2): 89-93.
This paper reports the measurement of five new sets of mid-infrared (MIR) laser magnetic resonance spectra (LMR) of the v 3 band (001-000) of 14 N16 O2 in its ground electronic state. It details the research background, experimental apparatus, and some results obtained. With the intracavity saturated absorption technique employed and the conditions of the phase sensitive modulation detection optimized, spectra of very high sensitivity and resolution have been obtained. These spectra are eligible for studying the structure and Zeeman property of 14 N16 O2 .
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INVERSION RECOVERY MEASUREMENTS: THE RADIATION DAMPING EFFECTS
LUO Huijun, WANG Fu, ZHU Peifen, PAN Tieying, SHI Xinmei
Chinese Journal of Magnetic Resonance, 2000, 17(2): 95-102.
In the presence of strong radiation damping, the conventional two-pulse inversion recovery measurements have been performed on water sample(90%H2 O/10%D2 O). It shows that if two pulses in IR sequence are 180° out of phase and the flip angle of the inversion pule is smaller than 180°, or if two pulses are in phase and the flip angle of the inversion pulse is larger than 180°, the signal intensity will continuously changes with the recovery time. Conversely, if two pulses are in phase (or 180° out of phase) and the flip angle of the inversion pulse is smaller than 180° (or larger than 180°), the signal intensity will jump from the negative maximum to the positive maximum around τ =T rd ln{tan[(π±δ)/2]}. Under the off-resonance condition, no matter what pulse phase, the beating effect can be always observed, but the phase of the signal explicitly depends on the relative phase of the pulses. As a result, the phase cycling will greatly suppress the beating effect. These phenomena can be well explained by the radiation damping theory. In addition, when the magnetization locates near the-zaxis during the detection, the deviation of theoretical expectation from the experimental data is closely related to the longitudinal relaxation effect.
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11 B VAS NMR AND 1 H MAS NMR STUDY ON THE BORON-CONTAINING ZEOLITES
CHEN Tiehong, SUN Pingchuan, DENG Feng, WANG Jingzhong, DING Datong
Chinese Journal of Magnetic Resonance, 2000, 17(2): 109-113.
The VAS (Variable Angle Spinning) NMR method was applied in the study on the Boron containing ZSM-12 and ZSM-5 zeolites. By the 11 B VAS NMR experiment and simulations of the powder patterns, the quadrupolar constant of the tri-coordinated boron was determined to be 2.4MHz, and the electrical field gradient coefficient 0.0. The resonance of the Boron-Silicon hydroxyl proton is at 2.3ppm, and by the 1 H{11 B} spin echo double resonance it is shown that the 2.3ppm protons are very weakly coupled with the boron atoms. Besides the 6.5ppm adsorbed water peak, a 2.7ppm water adsorption peak was also found, whose position is the same with the extra framework Al hydroxyls. This kind of water adsorption signal can be distinguished by the 1 H{27 Al} spin echo double resonance experiment.
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STUDY ON COMPUTATIONAL CHEMISTRY OF ELEMENE AND ITS DERIVATIVES I Theoretical Calculation of 13 C NMR Chemical Shifts of β-elemene
YE Jinxing, CHENG Guobao, HU Jiehan
Chinese Journal of Magnetic Resonance, 2000, 17(2): 115-120.
13 C NMR chemical shifts of a new drug for antitutor-β-elemene have been studied by quantum chemical calculation. The calculations both at the ab initio Hartree-Fock and B3LYP density function level of theory (6-31G* ) at the molecular mechanics MMX and Quantum chemistry RHF/6-31G* (or B3LYP/6-31G* ) optimized geometry have been implemented. Comparisons of both error analysis and linear correlation analysis have been performed between the theoretical and experimental chemical shifts. The results using GIAO gauge transformation method are better than those using CSGT method. The results using GIAO-B3LYP/6-31G* //B3LYP/6-31G* level are the best, with RMS of 4.3ppm, correlation coefficient R 2 of 0.998, SD of 2.42ppm. GIAO B3LYP/6-31G* //MMX is a good method of counterpoising between the computational expense and accuracy of results, with RMS of 4.9ppm, R 2 of 0.996, SD of 3.04ppm.