 can therefore be converted to frequency by `$\omega=s/\omega_{\beta,\gamma}$`.

The *half-width* of this peak, as a fraction of its location `$\omega_{\beta,\gamma}$`, is roughly `$1/P_{\beta,\gamma}$` where `$P_{\beta,\gamma}\equiv\sqrt{\beta\gamma}$`.

Frequency-domain symmetry, time-frequency concentration, and similarity to a Gaussian are all maximized near `$\gamma=3$`.  This means that the only parameter that needs to be adjusted is `$\beta$`.

Increasing `$\beta$` has the effect of increasing the nu