Show that the wavefunction Ψ(x) = N sin kx + iN cos kx is an eigen function of the momentum operator and determine its eigen value.
The momentum operator is "\\hat{p} =- i\\hbar\\dfrac{\\partial}{\\partial x}". By definition, the eigen function has the following property:
where "\\lambda" is the corresponding eigenvalue. Substituting the function and peforming the differentiation, obtain:
"\\hat{p}\\Psi(x) = - i\\hbar\\dfrac{\\partial}{\\partial x} (N\\sin(kx) + iN\\cos(kx)) = - i\\hbar(Nkcos(kx) - iNk\\sin(kx)) =\\\\\n=-i\\hbar Nkcos(kx) - \\hbar Nk\\sin(kx)"
Factoring out "-\\hbar k" , have:
Thus, this finction is indeed the eigen function of the momentum operator. Comparing the last equation with the first one, find the eigenvalue:
Answer. "\\Psi(x)" is the eigenfunction of the momentum operator with the eigenvalue "\\lambda = -\\hbar k".
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