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Two-electron atom
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Two-electron atom : ウィキペディア英語版
Two-electron atom
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.〔
: E\psi = -\hbar^2\left(+\nabla_2^2 \right) + \frac\nabla_1\cdot\nabla_2\right ) \psi + \frac\left(\frac+\frac \right) \right ) \psi
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
: |\bold_| = |\bold_2 - \bold_1 | \,\!
''μ'' is again the two-body reduced mass of an electron with respect to the nucleus of mass ''M'', so this time
: \mu = \frac \,\!
and ''Z'' is the atomic number for the element (not a quantum number).
The cross-term of two laplacians
:\frac\nabla_1\cdot\nabla_2\,\!
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:
: \psi = \psi(\bold_1,\bold_2)
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)
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