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In atomic physics, a two-electron atom or helium-like ion is a quantum mechanical system consisting of one nucleus with a charge of ''Ze'' and just two electrons. This is the first case of many-electron systems where the Pauli exclusion principle plays a central role. It is an example of a three-body problem. The first few two-electron atoms are: ==Schrödinger equation== The Schrödinger equation for any two-electron system, such as the neutral Helium atom (He, ''Z'' = 2), the negative Hydrogen ion (H−, ''Z'' = 1), or the positive Lithium ion (Li+, ''Z'' = 3) is:〔Physics of Atoms and Molecules, B.H. Bransden, C.J.Joachain, Longman, 1983, ISBN 0-582-44401-2〕 For a more rigorous mathematical derivation of Schrödinger's equation, see also.〔 : where r1 is the position of one electron (''r''1 = |r1| is its magnitude), r2 is the position of the other electron (''r''2 = |r2| is the magnitude), ''r''12 = |r12| is the magnitude of the separation between them given by : ''μ'' is again the two-body reduced mass of an electron with respect to the nucleus of mass ''M'', so this time : and ''Z'' is the atomic number for the element (not a quantum number). The cross-term of two laplacians : is known as the ''mass polarization term'', which arises due to the motion of atomic nuclei. The wavefunction is a function of the two electron's positions: : There is no closed form solution for this equation. 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「Two-electron atom」の詳細全文を読む スポンサード リンク
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