In two dimensions Schrodinger's equation takes the form
(1)
Because x and y appear in the equation, we must assume
is a function of both
and
If we assume that
is a product of a function of
with a function of
then
Substitution of this expression into (1) gives
![]()
Divide throughout by
to obtain
![]()
Rearrange to get![]()
and
are independent variables, independent of each other, The left hand side is a function of
only and the right hand side is a function of
only, so both sides must be equal to a constant
Ignoring the arbitrary constant
we can write
and![]()
Since
is arbitrary we can write
and
to obtain
and![]()
These two equations can be solved separately as for the one dimensional simple harmonic oscillator and the two solutions multiplied to give the general solution,
to (1) . The energy of oscillations in the
– direction is
and the energy corresponding to oscillations in the
– direction is
The total energy will be the sum of these:![]()