Asymmetry Lost

From the post "High Frequency EMW From Laser" dated 31 Jul 2015 and "It's All Fluorescence Outside, Inside" dated 29 Jul 2015, the cone provides the asymmetry that differentiate between a counter clockwise rotating particle generating a \(E\) field outwards and a clockwise rotating particle generating a \(E\) field inwards.  This asymmetry is lost when \(\small{\theta\to90^o}\),

Both clockwise and anti-clockwise rotations generate a \(E\) field parallel to \(PO\).  This radiation is distinct from EMW and photons.  Neither,

\(B=i\cfrac{\partial\,E}{\partial x}\)

nor

\(B=-i\cfrac{\partial\,E}{\partial x}\)

is applicable.  And occurs in a single burst as \(\small{v_{cir}\approx0}\) is swapped as \(\small{v_{shm}}\) on emission and the particle stopped oscillating, from the post "It's All Fluorescence Outside, Inside" dated 29 Jul 2015.

This is a short burst of \(E\) field towards \(O\).