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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 Landé g-factor ： ウィキペディア英語版 Landé g-factor In physics, the Landé ''g''-factor is a particular example of a ''g''-factor, namely for an electron with both spin and orbital angular momenta. It is named after Alfred Landé, who first described it in 1921. In atomic physics, the Landé ''g''-factor is a multiplicative term appearing in the expression for the energy levels of an atom in a weak magnetic field. The quantum states of electrons in atomic orbitals are normally degenerate in energy, with these degenerate states all sharing the same angular momentum. When the atom is placed in a weak magnetic field, however, the degeneracy is lifted. == Description == The factor comes about during the calculation of the first-order perturbation in the energy of an atom when a weak uniform magnetic field (that is, weak in comparison to the system's internal magnetic field) is applied to the system. Formally we can write the factor as, :$g\_J=\; g\_L\backslash frac+g\_S\backslash frac.$ The orbital ''g''-factor is equal to 1, and under the approximation $g\_S\; =\; 2$, the above expression simplifies to :$g\_J\; \backslash approx\; \backslash frac+\backslash frac.$ Here, ''J'' is the total electronic angular momentum, ''L'' is the orbital angular momentum, and ''S'' is the spin angular momentum. Because ''S''=1/2 for electrons, one often sees this formula written with 3/4 in place of ''S''(''S''+1). The quantities ''gL'' and ''gS'' are other ''g''-factors of an electron. If we wish to know the ''g''-factor for an atom with total atomic angular momentum F=I+J, :$g\_F=\; g\_J\backslash frac+g\_I\backslash frac$ :$\backslash approx\; g\_J\backslash frac$ This last approximation is justified because $g\_I$ is smaller than $g\_J$ by the ratio of the electron mass to the proton mass. 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「Landé g-factor」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.