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NMR excitation of quadrupolar order using adiabatic demagnetization in the rotating frame

机译:在旋转框架中使用绝热退磁对四极阶进行NMR激发

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Adiabatic demagnetization and remagnetization in the rotating frame (ADRF and ARRF) are shown to be practical and efficient techniques for exciting and observing quadrupolar order, T-2,T-0, in NMR of quadrupolar nuclei such as H-2 or Na-23. A detailed theoretical description of ADRF and ARRF of spin I=1 and 3/2 nuclei. based on the well-known vector model of NMR, is presented and used to derive analytically a variety of pulse shapes for ADRF and ARRF. This theory is also used to calculate the state of the spin I=1 and 3/2 density operators following an ADRF or ARRF pulse and it is shown that the desired coherence transfer processes have the maximum amplitudes allowed by the well-known "universal bound" theorem. In principle, therefore, ADRF is shown to be superior as a method of exciting quadrupolar order to the Jeener-Broekaert experiment since the latter fails to excite the maximum T-2,T-0 amplitude for spin I=3/2 nuclei. The performance of ADRF is investigated using computer calculations and simulations and the conditions under which it yields broadband (i.e., non-oscillatory) excitation of quadrupolar order are derived. Using both H-2 (I=1) and Na-23 (I=3/2) NMR of liquid crystalline and biological samples, ADRF and ARRF rut demonstrated experimentally. The predicted broadband excitation behavior is observed far both ADRF and ARRF, whereas both the Jeener-Broekaert and double-quantum filtration experiments show excitation profiles that oscillate sinusoidally as a function of either the quadrupolar splitting parameter, omega(Q), or the duration of the pulse sequence, tau. Finally, a more general discussion of ADRF and ARRF of quadrupolar nuclei is presented and it is shown that the maximum coherence transfer amplitudes are achieved for nuclei of any spin quantum number I. (C) 1998 American Institute of Physics. [S0021-9606(98)00103-2]. [References: 34]
机译:旋转框架(ADRF和ARRF)中的绝热退磁和复磁被证明是实用有效的技术,用于激发和观察四极核(如H-2或Na-23)中的四极阶T-2,T-0。 。自旋I = 1和3/2原子核的ADRF和ARRF的详细理论描述。提出了基于著名的NMR矢量模型的方法,并用于分析得出ADRF和ARRF的各种脉冲形状。该理论还用于计算ADRF或ARRF脉冲后自旋I = 1和3/2密度算符的状态,并且表明所需的相干传递过程具有众所周知的“通用界”所允许的最大幅度定理。因此,从原理上讲,ADRF作为激发四极级阶跃的方法优于Jeener-Broekaert实验,因为后者无法激发自旋I = 3/2核的最大T-2,T-0振幅。使用计算机计算和仿真研究了ADRF的性能,并推导了其产生四极阶宽带(即非振荡)激励的条件。使用液晶和生物样品的H-2(I = 1)和Na-23(I = 3/2)NMR,ADRF和ARRF车辙通过实验证明。在ADRF和ARRF上都观察到了预测的宽带激发行为,而Jeener-Broekaert和双量子过滤实验均显示出激发曲线以四极分裂参数ω(Q)或持续时间的函数呈正弦振荡。脉冲序列tau。最后,对四极核的ADRF和ARRF进行了更一般的讨论,结果表明,对于任何自旋量子数为I的核,其最大相干传递幅度都达到了。(C)1998美国物理研究所。 [S0021-9606(98)00103-2]。 [参考:34]

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