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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Electric field gradient ： ウィキペディア英語版 Electric field gradient In atomic, molecular, and solid-state physics, the electric field gradient (EFG) measures the rate of change of the electric field at an atomic nucleus generated by the electronic charge distribution and the other nuclei. The EFG couples with the nuclear electric quadrupole moment of quadrupolar nuclei (those with spin quantum number greater than one-half) to generate an effect which can be measured using several spectroscopic methods, such as nuclear magnetic resonance (NMR), electron paramagnetic resonance (EPR, ESR), nuclear quadrupole resonance (NQR), Mössbauer spectroscopy or perturbed angular correlation (PAC). The EFG is non-zero only if the charges surrounding the nucleus violate cubic symmetry and therefore generate an inhomogeneous electric field at the position of the nucleus. EFGs are highly sensitive to the electronic density in the immediate vicinity of a nucleus. This is because the EFG operator scales as ''r''−3, where ''r'' is the distance from a nucleus. This sensitivity has been used to study effects on charge distribution resulting from substitution, weak interactions, and charge transfer. ==Definition== A given charge distribution of electrons and nuclei, ''ρ''(r), generates an electrostatic potential ''V''(r). The derivative of this potential is the negative of the electric field generated. The first derivatives of the field, or the second derivatives of the potential, is the electric field gradient. The nine components of the EFG are thus defined as the second spatial derivatives of the electrostatic potential, evaluated at the position of a nucleus: :$V\_\; =\; \backslash frac.$ For each nucleus, the components ''Vij'' are combined as a symmetric 3 × 3 matrix. Under the assumption that the charge distribution generating the electrostatic potential is external to the nucleus, the matrix is traceless, for in that situation Laplace's equation, ∇2''V''(r) = 0, holds. Relaxing this assumption, a more general form of the EFG tensor which retains the symmetry and traceless character is :$\backslash varphi\_=V\_-\backslash frac\backslash delta\_\backslash nabla^2V,$ where ∇2''V''(r) is evaluated at a given nucleus. As ''V'' (and ''φ'') is symmetric it can be diagonalized. The principal tensor components are usually denoted ''Vzz'', ''Vyy'' and ''Vxx'' in order of decreasing modulus. Given the traceless character, only two of the principal components are independent. Typically these are described by ''Vzz'' and the asymmetry parameter, ''η'', defined as :$$ \eta = \frac} \vert \geq \vert V_ \vert \geq \vert V_ \vert and $V\_\; +\; V\_\; +\; V\_=0$, thus $0\; \backslash leq\; \backslash eta\; \backslash leq\; 1$. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Electric field gradient」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.