Now we will consider a one-dimensional field in which the potential V is everywhere 0 except on the interval [0;L] where the potential energy of a particle is negative with constant value U0 < 0. Intervals like this are said one-dimensional potential wells with depth U0.
In Classical Mechanics a particle with positions 0<x<L and total energy lesser than 0 but greater than U0 can not escape from the well because outside it its kinetic energy K = -0 would be negative.
The Quantum Mechanics approach is the following:
if 0<x<L the wave function must be a solution of the equation (the subscript I stands for 'Internal')
if x<0 or x>L the wave function must be a solution of the equation (the subscript E stands for 'External')
Since the wave function must be continuous and differentiable in the entire field, for x=0 or x= L the two solutions and their derivatives must have the same values.
Moreover, since the Quantum Mechanics approach must asymptotically converge to Classical Mechanics, x→±∞ ⇒ ψ → 0.
With a method similar to that taken in the previous section 8, we assume for the equation (9.1) a solution and, in the same way we obtain
But in this case, we cannot assume the boundary conditions ψ(0)=0 e ψ(L)=0, because the walls of the pit have finite altitude. So, for now, we have
Solutions of (9.2) can not be something like , because the second derivative implies a negative value to the the square of b. If we otherwise assume solutions like ψ(x) = a eb x, differentiating twice with respect to x we have
and the comparison with (9.2) gives
This equality is acceptable because, by hypothesis, is negative. Therefore outside the well the function may have the form
Since the wave function must be zero for x→±∞, we assume (the subscript EL stands for 'External Left' and the subscript ER stands for 'External Right' )
For x=0 the two solutions and their derivatives must be equal. So
The same happens for x=L. So
From (9.6) and (9.8) we have
Finally, using the values of c and kI from (9.3) and (9.7), we have
By solving this equation with respect to for each value of n we can obtain the energy levels inside the well. There is no analytical way to calculate thise solutions, but they can be approximated at will with a numerical method beginning from n=1 and raising it while negative solutions are found.
JS uses the simple bisection algorithm. The code is in the HTML source of this page.