Fig. 3

\(\:\frac{A}{{v}_{m}}\) as well as \(\:\frac{R}{{t}_{m}}\) versus \(\:\frac{{\tau}_{a}}{{t}_{s}}\left(=\frac{{\tau}_{a}}{{t}_{m}\sqrt{2}}\right)\) on log-log scale: (a) and (b), respectively for \(\:{\omega}_{o}={10}^{6}Hz\), \(\:{\tau}_{a}=70\mu s\).