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从应用于电子自旋回波包络调制(ESEEM)的频率和幅度快速构建固态磁共振粉末光谱。

Rapid construction of solid-state magnetic resonance powder spectra from frequencies and amplitudes as applied to ESEEM.

作者信息

Stoll Stefan, Schweiger Arthur

机构信息

Physical Chemistry Laboratory, ETH Zürich, CH-8093 Zürich, Switzerland.

出版信息

J Magn Reson. 2003 Aug;163(2):248-56. doi: 10.1016/s1090-7807(03)00120-4.

Abstract

In many Fourier-transform spectroscopies, such as pulse magnetic resonance (NMR, EPR), time-domain signals are acquired. Parameters are extracted from these signals by fitting numerical simulations to the experimental data. At present, simulations are often performed in frequency domain (FD). These computations generate a list of frequencies and amplitudes associated with the complex exponential components evolving during one or several variable time intervals. In order to compare simulations with experiments, this peak list is converted to a finite-length time-domain (TD) signal. This can be achieved either by directly evoluting the exponentials in time (direct method) or by rounding their frequencies and binning their amplitudes into a frequency-domain array (histogram method). The first approach is equivalent to a brute-force TD simulation and is slow for a large number of peaks. The second approach is a fast, but very crude approximation and is usually applied without considering in detail the errors involved. A third method introduced and illustrated here is based on the convolution and deconvolution of a short finite impulse response filter kernel. This convolution approach is much faster than the direct method and by orders of magnitude more accurate than the histogram method. For both TD and FD signals a detailed analysis of the errors and of the associated computational costs is presented. The convolution approach is applicable to any simulation problem where TD signals consist of a large number of complex exponentials. In particular, it is the method of choice for simulating 1D and 2D electron spin echo envelope modulation (ESEEM) spectra of disordered systems.

摘要

在许多傅里叶变换光谱学中,如脉冲磁共振(核磁共振、电子顺磁共振),会采集时域信号。通过将数值模拟与实验数据拟合,从这些信号中提取参数。目前,模拟通常在频域(FD)中进行。这些计算会生成与在一个或几个可变时间间隔内演化的复指数分量相关的频率和幅度列表。为了将模拟与实验进行比较,这个峰值列表会被转换为有限长度的时域(TD)信号。这可以通过在时间上直接演化指数(直接方法)或通过对其频率进行舍入并将其幅度归入频域数组(直方图方法)来实现。第一种方法等同于强力时域模拟,对于大量峰值来说速度很慢。第二种方法速度快,但非常粗略,通常在不详细考虑所涉及误差的情况下应用。这里介绍并说明的第三种方法基于短有限脉冲响应滤波器内核的卷积和解卷积。这种卷积方法比直接方法快得多,并且比直方图方法精确几个数量级。对于时域和频域信号,都给出了对误差和相关计算成本的详细分析。卷积方法适用于任何时域信号由大量复指数组成的模拟问题。特别是,它是模拟无序系统的一维和二维电子自旋回波包络调制(ESEEM)光谱的首选方法。

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