Question
Prove that the Hermite functions $\psi_{n}=N_{n} e^{-v^{2} / 2} H_{n}(y)$ are orthogonal and show that the normalization constant which makes $\int_{-\infty}^{\infty} \psi_{n}^{2}(x) d x=$ 1 is$$N_{n}=\left(\frac{\alpha}{\sqrt{\pi} 2^{n} n !}\right)^{\prime}$$
Step 1
Step 1: The Hermite functions are defined as $\psi_{n}=N_{n} e^{-v^{2} / 2} H_{n}(y)$, where $H_{n}(y)$ are the Hermite polynomials and $N_{n}$ is the normalization constant. Show more…
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