Single Electron Atom Wave Functions
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Schrödinger Equation
The Schrödinger equation describing an electron in a central
field is of the form
![[Graphics:../Images/hwavefunctions_gr_30.gif]](../Images/hwavefunctions_gr_30.gif)
In the scaled coordinates that we are using,
and ,
where
is the nuclear charge. The Schrödinger equation for an attractive
Coulomb potential, ,
is
![[Graphics:../Images/hwavefunctions_gr_35.gif]](../Images/hwavefunctions_gr_35.gif)
The standard add-on package Calculus`VectorAnalysis`
has commands for representing the various vector differential operators
in a number of coordinate systems. First load the package.
![[Graphics:../Images/hwavefunctions_gr_36.gif]](../Images/hwavefunctions_gr_36.gif)
Now define a Schrödinger operator,
![[Graphics:../Images/hwavefunctions_gr_37.gif]](../Images/hwavefunctions_gr_37.gif)
Set the default coordinate system for the functions from Calculus`VectorAnalysis`
to be spherical polar coordinates:
![[Graphics:../Images/hwavefunctions_gr_38.gif]](../Images/hwavefunctions_gr_38.gif)
Now check to see if
is an eigenfunction of the Schrödinger operator.
![[Graphics:../Images/hwavefunctions_gr_40.gif]](../Images/hwavefunctions_gr_40.gif)
![[Graphics:../Images/hwavefunctions_gr_41.gif]](../Images/hwavefunctions_gr_41.gif)
This of course agrees with the known eigenvalues for the energy
of this system: .
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