Factor $1/\sqrt{2\pi}$ in the normalization of wave function packet My book has started using the wave packet definition as follows (time independent form):
$$\Psi(x) = \frac{1}{\sqrt{2\pi}}\int_{-\infty}^{\infty} A(k) \ e^{ikx}dx$$
I do not understand where the $1/\sqrt{2\pi}$ comes from in this definition.  First, I thought it has something to do with normalization however, I can't seem to prove this to myself.
$$\Psi'(x) = N \int_{-\infty}^{\infty} A(k) \ e^{ikx}dx$$
$$\Psi'(x)^{\ast} = N \int_{-\infty}^{\infty} A^{\ast}(k) \ e^{-ikx}dx$$
$$\Psi'(x) \Psi'(x)^{\ast}= N^2  \int_{-\infty}^{\infty} A(k) \ e^{ikx}dx \int_{-\infty}^{\infty} A^{\ast}(k) \ e^{-ikx}dx = N^2 \int_{-\infty}^{\infty} A(k) A^{\ast}(k)dx = N^2 A(k) A^{\ast}(k)$$
The last step I justify by the conditions that the wave functions must approach zero as you go from $\pm \infty$.
$$P = 1 = N^2 \int_{-\infty}^{\infty} A(k) A^{\ast}(k)dk$$
I am not sure where to go from here. Does this term actually come from the normalization? If so, how can I show this.
 A: The Fourier-transform operators
$$
\hat F = \int \mathrm dx \frac{e^{ikx}}{\sqrt{2\pi}}
\qquad
\hat F{}^{-1} = \int \mathrm dk \frac{e^{-ikx}}{\sqrt{2\pi}}
$$
are prettier if you attach a $\sqrt{2\pi}$ to them both, instead of the asymmetric
$$
\hat F_\text{ugly} = \int \mathrm dx \ {e^{ikx}}
\qquad
\hat F{}_\text{ugly}^{-1} = \int \mathrm dk \frac{e^{-ikx}}{{2\pi}}
$$
You should think of $\Psi(x) = \hat F {}^{-1} A(k)$ as your wavefunction, but $A(k) = \hat F\Psi(x)$ as also your wavefunction, in momentum space. You’re currently stuck because the normalization of $\Psi$ is related to the normalization of $A$.
Perhaps abetting your confusion: in the current version of your question (v3), you erroneously have $\Psi(x) = \hat F A(k)$. That’s impossible, because the integral on the right side eats up the dummy variable $x$, so the left side should be a function of $k$.
Likewise you have to be careful about the dummy variables when you are computing your overlap integrals.  You expect that
\begin{align}
1 = \left< \Psi | \Psi \right>
&= \int \mathrm dx\ \Psi^*(x) \Psi(x)
\\ 
&= \int \mathrm dx
\left(
\int\mathrm dk A^*(k) \frac{e^{+ikx}}{\sqrt{2\pi}}
\right)
\left(
\int\mathrm dk’ A(k’) \frac{e^{-ik’x}}{\sqrt{2\pi}}
\right)
\end{align}
You’re going to exploit
$ \int\mathrm dx\ e^{i(k-k’)x} \sim \delta(k-k’)
$
and get rid of two of the integrals, leaving you with
$$
1= \left<\Psi|\Psi\right>_x = \left<A|A\right>_k
$$
which is what I meant about the normalizations being related.  But you’re going to look up and/or prove that there are the correct amount of $\sqrt{2\pi}$ involved, rather than trusting my one-squiggle relationship.
If you have been putting off reading about Fourier transforms, today is a good day.
A: For normalization, you want to look at $\int\psi^*\psi\,\text dx=1$. Try this and the result will be much better.
