Part (b) shows that the transform of is with of degree . Part (c) shows that it solves the same eigenvalue equation as , with the same . The assumed uniqueness of the polynomial solution of each degree therefore forces ; hence .
The constants can also be determined. Substituting into the equation gives the Hermite differential equation
Comparison of the leading coefficient yields . If the leading coefficient of is , part (b) gives leading coefficient for . Thus
Thus Hermite functions are Fourier eigenfunctions with the paper's unnormalized Fourier transform; dividing that transform by gives the unitary eigenvalues .

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