If we express \(f_{res}\) in terms of \(a_{\psi}\), the extend of \(\psi\),
\(a_{\psi}=\cfrac{\pi \sqrt { 2{ mc^{ 2 } } } }{G}\)
\(f_{res}=\cfrac{sech(\pi)}{2\pi}\cfrac{G}{\sqrt{m}}=\cfrac { sech(\pi ) }{ 2 } \cfrac { \sqrt { 2{ c^{ 2 } } } }{ a_{\psi} } \)
\(f_{res}=\cfrac { \sqrt { 2 } }{ 2 } sech(\pi )\cfrac { c }{ a_{\psi} }\)
\(f_{res}=0.061\cfrac { c }{ a_{\psi} }\)
Does the system work in reverse? Once \(\psi\) is set into resonance, and \(f_{res}\) is reduced does \(a_{\psi}\) increases.
Can a shield be projected forward by suddenly decreasing \(f_{res}\) and turning off. In effect, an energy density \(\psi\) projectile.
And I continue to dream anime... 看\(\psi\)！
