eljose
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let be the next problem: given a particle with mass so \hbar=(2m)^{0.5} then we would have the quantum Hamiltonian:
H\phi(x)=E_{n}\phi(x) with H=-D^{2}\phi+V(x)\phi
my question is how i would choose the potential so we have that the energies are the root of the equation f(x)=0
i try using the WKB approach to calculate the function:
\phi(x)=e^{iS(x)/\hbar} with s^{2}=E_{n}-V(x)
with that i get a functional equation for the potential V(x), my problem is how i introduce the condition that the energies are the roots of f(x)...

H\phi(x)=E_{n}\phi(x) with H=-D^{2}\phi+V(x)\phi
my question is how i would choose the potential so we have that the energies are the root of the equation f(x)=0
i try using the WKB approach to calculate the function:
\phi(x)=e^{iS(x)/\hbar} with s^{2}=E_{n}-V(x)
with that i get a functional equation for the potential V(x), my problem is how i introduce the condition that the energies are the roots of f(x)...

