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Two-electron atom

From Wikipedia, the free encyclopedia

Helium-like quantum systems that have a nucleus and two electrons

Inatomic physics, atwo-electron atom orhelium-like ion is aquantum mechanical system consisting of onenucleus with acharge ofZe and just twoelectrons. This is the first case of many-electron systems where thePauli exclusion principle plays a central role.

It is an example of athree-body problem.

The first few two-electron atoms are:

Z = 1:Hhydrogen anion
Z = 2:Hehelium atom
Z = 3:Li+lithium ion
Z = 4:Be2+beryllium ion
Z = 5:B3+boron ion

Schrödinger equation

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The Schrödinger equation for any two-electron system, such as the neutralHelium atom (He,Z = 2), the negativeHydrogenion (H,Z = 1), or the positiveLithium ion (Li+,Z = 3) is:[1] For a more rigorous mathematical derivation of the Schrödinger equation, see also.[1]Eψ=2[12μ(12+22)+1M12]ψ+e24πε0[1r12Z(1r1+1r2)]ψ{\displaystyle E\psi =-\hbar ^{2}\left[{\frac {1}{2\mu }}\left(\nabla _{1}^{2}+\nabla _{2}^{2}\right)+{\frac {1}{M}}\nabla _{1}\cdot \nabla _{2}\right]\psi +{\frac {e^{2}}{4\pi \varepsilon _{0}}}\left[{\frac {1}{r_{12}}}-Z\left({\frac {1}{r_{1}}}+{\frac {1}{r_{2}}}\right)\right]\psi }wherer1 is the position of one electron (r1 = |r1| is its magnitude),r2 is the position of the other electron (r2 = |r2| is the magnitude),r12 = |r12| is the magnitude of the separation between them given by|r12|=|r2r1|{\displaystyle |\mathbf {r} _{12}|=|\mathbf {r} _{2}-\mathbf {r} _{1}|}μ is the two-body reduced mass of an electron with respect to the nucleus of massMμ=meMme+M{\displaystyle \mu ={\frac {m_{\text{e}}M}{m_{\text{e}}+M}}}andZ is theatomic number for the element (not aquantum number).

The cross-term of two Laplacians1M12{\displaystyle {\frac {1}{M}}\nabla _{1}\cdot \nabla _{2}}is known as themass polarization term, which arises due to the motion ofatomic nuclei. The wavefunction is a function of the two electron's positions:ψ=ψ(r1,r2){\displaystyle \psi =\psi (\mathbf {r} _{1},\mathbf {r} _{2})}

There is no closed form solution for this equation.

Spectrum

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The optical spectrum of the two electron atom has two systems of lines. A para system of single lines, and an ortho system of triplets (closely spaced group of three lines). The energy levels in the atom for the single lines are indicated by1S01P11D21F3 etc., and for the triplets, some energy levels are split:3S13P23P13P03D33D23D13F43F33F2.[2]Alkaline earths andmercury also have spectra with similar features, due to the two outer valence electrons.[2]

See also

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References

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  1. ^abBransden, B. H.; Joachain, C. J. (1983).Physics of Atoms and Molecules. Longman.ISBN 0-582-44401-2.
  2. ^abHerzberg, Gerhard; J W T Spinks (1944).Atomic Spectra and Atomic Structure (2nd ed.). New York:Dover Publications. p. 75.
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