首页> 外文期刊>Collection of Czechoslovak Chemical Communications >A SIMPLE NUMERICAL METHOD FOR CALCULATING GAUSSIAN NMR SPECTRAL LINE SHAPES PARTIALLY NARROWED DUE TO A MOTION WITH THE EXPONENTIAL SPECTRAL AUTOCORRELATION FUNCTION
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A SIMPLE NUMERICAL METHOD FOR CALCULATING GAUSSIAN NMR SPECTRAL LINE SHAPES PARTIALLY NARROWED DUE TO A MOTION WITH THE EXPONENTIAL SPECTRAL AUTOCORRELATION FUNCTION

机译:计算具有指数谱自相关函数的运动导致部分变窄的高斯NMR谱线形状的一种简单数值方法

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摘要

A simple numerical method for calculating NMR spectral line shapes resulting from a Gaussian line by a partial narrowing due to a motion with the exponential spectral autocorrelation function of the form exp was developed. It was found that the partially narrowed line is narrower not only than the parent Gaussian line with the second moment of epsilon_p~2 but also than the Lorentzian line with the half-width of 2epsilon_p~2i_c obtained from the extreme narrowing approximation. The central intensity increase compared with the closer of these two lines is less than 50.2%. Asymptotic developments for large values of epsilon - epsilon_o and for large values of epsilon_pi_c were derived. Two-term approximation applied to the extreme narrowing case led to a very simple modification of the Lorentzian line having the correct second moment epsilon_p~2. Analysis of this modified Lorentzian line showed that attempts to estimate epsilon_p~2 from truncated second moments of Lorentzian lines without knowledge of i_c are hopeless. The case of the poly exponential spectral autocorrelation function with all but one correlation times fast enough to allow for the extreme narrowing, modelling the case of an anisotropic motion, is also considered.
机译:开发了一种简单的数值方法,用于计算高斯线由于运动引起的局部变窄而产生的NMR谱线形状,其形式为exp的指数谱自相关函数。结果发现,部分变窄的线不仅比具有第二个epsilon_p〜2矩的母高斯线更窄,而且比由极窄化近似得到的具有半个宽度2epsilon_p〜2i_c的洛伦兹线更窄。与这两条线中较近的一条相比,中心强度增加小于50.2%。得出了大的epsilon-epsilon_o和大的epsilon_pi_c的渐近发展。应用于极端变窄情况的二项近似导致对具有正确的第二矩epsilon_p〜2的洛伦兹线的非常简单的修改。对这一修改后的洛伦兹线的分析表明,在不知道i_c的情况下,试图从截断的洛伦兹线的第二时刻估计epsilon_p〜2是没有希望的。还考虑了多指数光谱自相关函数的情况,除了一个相关时间外,所有其他时间都足够快以允许极端变窄,从而模拟了各向异性运动的情况。

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