1. We first prove orthogonality of non-degenerate eigenvectors of the Hamiltonian. Consider the braket and act with the Hamiltonian in both directions,

   $ \left\langle\alpha | H |\beta\right\rangle = E_\alpha\left\langle\alpha |\beta\right\rangle = E _\beta\left\langle\alpha |\beta\right\rangle $

   If the states are not orthogonal ($\left\langle\alpha |\beta\right\rangle \neq 0 $) then we would get a contradiction since we assume the states are non-degenerate ($E_\alpha\neq E_\beta $). So we must have

   $\left\langle\alpha |\beta\right\rangle = 0 $

   for distinct states.

2. Now we need to prove that the braket of two eigenstates is equal to $1$ up to a phase. Consider the braket:

   $ \left\langle\alpha |\alpha\right\rangle = \sum_n \left\langle\alpha |n\right\rangle \left\langle n |\alpha\right\rangle = \left\langle\alpha |\alpha\right\rangle \left\langle\alpha |\alpha\right\rangle $

   where we have inserted a sum over the states of the Hamiltonian and then used the orthogonality relation that we proved above. Now we can divide both sides by $\left\langle\alpha |\alpha\right\rangle $ to get

   $\left\langle\alpha |\alpha\right\rangle = 1 $

3. Thus for we have only considered non-degenerate eigenvectors. Degenerate eigenvectors can't be distinguished and they don't need to be orthogonal to each other. However, for any set of linearly independent vectors (all wavefunctions of a Hamiltonian are linearly independent) there exists linear combinations of them that are orthogonal which can be found through the Gram–Schmidt procedure. Thus one can choose the vectors to be linearly independent.

We first prove orthogonality of non-degenerate eigenvectors of the Hamiltonian. Consider the braket and act with the Hamiltonian in both directions,

$ \left\langle\alpha | H |\beta\right\rangle = E_\alpha\left\langle\alpha |\beta\right\rangle = E _\beta\left\langle\alpha |\beta\right\rangle $

If the states are not orthogonal ($\left\langle\alpha |\beta\right\rangle \neq 0 $) then we would get a contradiction since we assume the states are non-degenerate ($E_\alpha\neq E_\beta $). So we must have

$\left\langle\alpha |\beta\right\rangle = 0 $

for distinct states.

2. Now we need to prove that the braket of two eigenstates is equal to $1$ up to a phase. Consider the braket:

$ \left\langle\alpha |\alpha\right\rangle = \sum_n \left\langle\alpha |n\right\rangle \left\langle n |\alpha\right\rangle = \left\langle\alpha |\alpha\right\rangle \left\langle\alpha |\alpha\right\rangle $

where we have inserted a sum over the states of the Hamiltonian and then used the orthogonality relation that we proved above. Now we can divide both sides by $\left\langle\alpha |\alpha\right\rangle $ to get

$\left\langle\alpha |\alpha\right\rangle = 1 $