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(14)N(I = 1)电子自旋回波包络调制的一般分析。

General analysis of (14)N (I = 1) electron spin echo envelope modulation.

作者信息

Lee H I, Doan P E, Hoffman B M

机构信息

Department of Chemistry, Northwestern University, Evanston, Illinois, 60208, USA.

出版信息

J Magn Reson. 1999 Sep;140(1):91-107. doi: 10.1006/jmre.1999.1803.

Abstract

The analysis methods described to date for (14)N electron spin echo envelope modulation (ESEEM) mostly deal with isotropic g- and (14)N hyperfine coupling tensors. However, many cases of rhombic tensors are encountered. In the present report we present general equations for analyzing orientation-selective ESEEM and illustrate their use. (i) We present general equations for the nuclear interactions in an electron spin system where the EPR signal arises from an isolated Kramers doublet, then give the nuclear (electron-nuclear double resonance) frequencies for I = 1 associated with such a system. (ii) These are incorporated into equations for single-crystal ESEEM amplitudes, which in turn are incorporated into general equations for the orientation-selective ESEEM that arises when the EPR envelope of a frozen-solution (powder) sample is determined by g anisotropy. (iii) This development is first used in the simplest limit of an isotropic g-tensor and leads to a more general picture of the response of the I = 1 modulation amplitude to variations in the nuclear hyperfine and quadrupole coupling constants, relative to the nuclear Zeeman interaction, than had been presented previously. We find that strong modulation occurs not only in the well-known regime where the "exact/near cancellation" condition (A/2 approximately nu(N)) is satisfied, but also when the nuclear hyperfine interaction is much larger than the nuclear Zeeman interaction (A/nu(N) > 3) with A/K = 4 approximately 5. (iv) We then describe the orientation-selective (14)N ESEEM frequency-domain patterns (g vs frequency) in the presence of anisotropic (rhombic) hyperfine and electron Zeeman interactions for both coaxial and noncoaxial cases. We derive analytical solutions when the g-, hyperfine, and nuclear quadrupole tensors are coaxial. (v) The method is applied to the ESEEM of the nitrogenase MoFe protein (Av1) to determine the full hyperfine and nuclear quadrupole tensors of (14)N nuclei interacting with the S = 32 FeMo-cofactor (Fe(7)S(8)Mo: homocitrate).

摘要

迄今为止所描述的用于(14)N电子自旋回波包络调制(ESEEM)的分析方法大多处理各向同性的g张量和(14)N超精细耦合张量。然而,会遇到许多菱形张量的情况。在本报告中,我们给出了用于分析取向选择性ESEEM的通用方程并说明其用法。(i)我们给出了电子自旋系统中核相互作用的通用方程,其中EPR信号源于孤立的克莱默斯二重态,然后给出与该系统相关的I = 1的核(电子 - 核双共振)频率。(ii)将这些纳入单晶ESEEM振幅方程,这些方程又被纳入当冷冻溶液(粉末)样品的EPR包络由g各向异性决定时出现的取向选择性ESEEM的通用方程。(iii)这一进展首先用于各向同性g张量的最简单极限情况,相对于核塞曼相互作用,得出了I = 1调制振幅对核超精细和四极耦合常数变化响应的更通用图像,这比之前所呈现的更为全面。我们发现,强调制不仅发生在满足“精确/近抵消”条件(A/2≈ν(N))的众所周知的情况下,而且当核超精细相互作用远大于核塞曼相互作用(A/ν(N)> 3)且A/K = 4≈5时也会发生。(iv)然后,我们描述了在存在各向异性(菱形)超精细和电子塞曼相互作用的情况下,同轴和非同轴情况下的取向选择性(14)N ESEEM频域模式(g与频率)。当g张量、超精细张量和核四极张量同轴时,我们推导了解析解。(v)该方法应用于固氮酶MoFe蛋白(Av1)的ESEEM,以确定与S = 32的FeMo - 辅因子(Fe(7)S(8)Mo:高柠檬酸)相互作用的(14)N核的完整超精细和核四极张量。

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