Physics, 16.05.2021 18:10 foralways3178
Prove that eigenfunctions of hamiltonian H = −(h/2m)(d^2/dx^2)+V(x) (the hamiltonian operator for a particle of mass m moving in one dimension) have defined parity in the case where energy is a function of position V (x) = V (−x).
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Prove that eigenfunctions of hamiltonian H = −(h/2m)(d^2/dx^2)+V(x) (the hamiltonian operator for a...
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