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The Hydrogen atom Fine structure

The Hydrogen atom Fine structure

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<strong>The</strong> <strong>Hydrogen</strong> <strong>atom</strong><br />

<strong>Fine</strong> <strong>structure</strong>


Relativistic effect – the Klein-Gordon<br />

equation<br />

the fine <strong>structure</strong> constant


• s=1/2<br />

<strong>The</strong> spin of the electron


<strong>The</strong> Dirac equation<br />

and act only on the spin<br />

<strong>The</strong> solution for hydrogen


• <strong>The</strong> total angular momentum<br />

• <strong>The</strong> energy depends on j!<br />

• Second-order approximation


Stationary perturbational method


<strong>The</strong> perturbational treatment of the<br />

relativistic effect<br />

If the Dirac equation is expanded in terms of v 2 /c 2 , one<br />

obtains 3 correction terms:<br />

• the relativistic correction of the kinetic energy<br />

• the Darwin-term (only for l=0)<br />

• the spin-orbit interaction term


Perturbation theory for a degenerate level<br />

Is desirable that the perturbation LS to be diagonal<br />

This is valid in the representation |lsjm j >,<br />

because L 2 , S 2 , J 2 and J z commute with LS.<br />

We write the scalar product as


<strong>The</strong> diagonal matrix element is<br />

It can be calculated analytically<br />

Finally


Adding these contributions, the terms depending on l<br />

cancel out.


<strong>The</strong> difference between the two splitted levels (the spinorbit<br />

splitting)


Lamb shift – quantum field theory


<strong>The</strong> Lamb shift experiment


Slight changes in the electromagnetic force


Hyperfine splitting<br />

• <strong>The</strong> magnetic momentum of the nucleus<br />

• <strong>The</strong> interaction with the magnetic moment of the<br />

electron (for l=0)<br />

• <strong>The</strong> splitting<br />

• For the ground state


Isotope shift (different reduced mass)

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