Image:Stark splitting in hydrogen.png
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[edit] Summary
This graph shows the energy eigenvalues of Stark shifts in hydrogen, as a function of electric field strength. Magnetic quantum number: |m| = 1, parabolic quantum number: (n1 − n2) = -n+4,-n+2,...,n-2,n-4; states with higher principle quantum number n experience a greater energy shift for a given electric field strength.
For large field strengths, energy eigenvalues do not actually cross; rather, the solutions are given by the Mathieu functions.
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Source: Created using MATLAB 6.5
Date: 16/3/2006
Author: Jeffrey Philippson
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- (del) (cur) 01:52, 17 March 2006 . . DJIndica (Talk | contribs) . . 1201×900 (21,052 bytes) (Description: Second order Stark shifts in hydrogen. Magnetic quantum number: |m| = 1, parabolic quantum number: (n1 − n2) = -n+4,-n+2,...,n-2,n-4; states with higher principle quantum number n experience a greater energy shift for a given electric fiel)
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