As shown at https://quantummechanics.ucsd.edu/ph130a/130_notes/node124.html from quantum physics by Jim Branson (2003), using separation of variables we can break up the general Schrodinger equation into:
- a time-only part that does not depend on space and does not depend on the potential
- a space-only part that does not depend on time:Since this is the only non-trivial part, unlike the time part which is trivial, this spacial part is just called "the time-independent Schrodinger equation".Note that the here is not the same as the in the time-dependent Schrodinger equation of course, as that psi is the result of the multiplication of the time and space parts. This is a bit of imprecise terminology, but hey, physics.
The key initial example to have in mind is the time independent Schrodinger equation for a free one dimensional particle.
Then, just like in solving partial differential equations with the Fourier series of the heat equation, the boundary conditions may make it so that only certain discrete values of
Eare possible solutions.
Then, the time part o the equation can be solved explicitly in the general case, as it does not depend on the potential , and it is just an exponential.
Therefore, all we need to do to solve the general Schrodinger equation is to solve the time-independent version, and then decompose the initial condition in terms of it like as done in Section "Solving partial differential equations with the Fourier series".
- we immediately see from the equation that the time-independent solutions are states of deterministic energy because the energy is an eigenvalue of the Hamiltonian operator
- the probability density of such a state does not change with time because the exponential time part cancels out on the conjugate