I am struggling to answer the following question:
Let ψ₁(x) and ψ₂(x) be normalisable energy eigenfunctions for a particle of mass m in one dimension moving in a potential V(x). Suppose that ψ₁ and ψ₂ have the same energy eigenvalue E. By considering ψ₁ψ₂' - ψ₂ψ₁', show that these wavefunctions must be proportional to one another.
I tried differentiating the Schrödinger equations and multiplying them together appropriately, but this just yielded a lot of messy algebra with no useful outcome.
I'm also wondering if there is a physical interpretation of this? Does it mean that the wavefunction for a normalisable energy eigenstate in one dimension always be chosen to be real?