If a quantum particle of mass m with the Hamiltonian operator H = (-h^2/(2m))d^2/dx^2 has the wave function W(x) = sin(3 Pi x/2), then its (eigen) energy is
The wavefunction for a given physical system contains the measurable information about the system. Solutions exist for the time independent Schrodinger equation only for certain values of energy, and these values are called "eigenvalues*" of energy. ...
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