I think the main problem is you claim the field inside the cone is opposite in phase to the field outside the cone because the colors are at opposite ends of the A/M scale,
as if the monopole was one phase and the radials act like a mirror keeping the field from the monopole inside the cone while allowing an opposite phase current to flow outside the cone,
That’s not how i see it,
let me explain what i think is going on until somebody proves otherwise,
The monopole and radial are in opposite phase with fields from both rotating in opposite directions, as seen in Henry’s FEKO plot,
That causes the fields between the radials and monopole to be either moving away from you or moving towards you depending on which side of the monopole we are looking at,
in the same way rollers on an old mangle rotate in opposite directions but from your perspective looking between the rollers they both move towards or away from you depending on which direction you crank the handle or which side of the mangle you look at ( mind you don’t trap your fingers )
The field seen on the outside of a radial is the same field as on the inside of a radial but moving in the opposite direction from your perspective like a single mangle roller,
The field seen on the outside is the leftover radiation after cancellation due to the opposite rotating fields interacting and cancelling and maybe some small leakage due to the radials not been parallel with the monopole,
The magnitude of that radiation is highest towards the top of the cone where the radials are furthest away from the monopole ( at a voltage not current maxima ) and lowest towards the base ( current maxima ) where the radials are closest and cancellation is more complete,
its not a 1/2wave current pattern on a 1/4wave radial caused by a current source at each end of the 1/4wave radial as you imagine,
Its clear to see that the magnitude of the radiation is only a small fraction of the radiation from the upper 1/2wave,
Which gets us back to gain,
Think about a collinear, say 2x 1/2wave phased with a 180 degree stub like the collinear j-pole,
You will never get close to the theoretical 3db over a dipole unless you put significant distance between the two 1/2wave radiators, and that’s using two radiators with very similar radiation field strengths,
As you reduce the separation between the two 1/2wave elements gain drops towards 2dbd,
How is it possible to have 2dbd from a vector when you have 1x 1/2wave radiator and only some very small magnitude of radiation from the cone that is in no way comparable to radiation from a second 1/2wave radiator?
That seems to defy the laws of physics,
Not only that but extending the radiator causes current phase in the cone area to shift resulting in a reduction in low angle radiation and an increase in high angle radiation just like a 5/8wave j-pole,
http://www.hamradio.me/antennas/58-wave-j-pole-vs-12-wave-j-pole-eznec-shootout.html
giving us less signal where we want it on the horizon,
You already told us peak signals come when the hoop is close to the zero crossing point using 1/4wave radials which is when you have an electrical 1/2wave above the cone, that gives us the best balance at the top of the cone, least radiation from the cone,
Its clear as mud that Avanti and the 90” radial clones did not optimise the design,
Its also clear the 7/8 monopole versions with 90” radials were even further from optimal,
That’s why we can adjust our antennas and make them perform better out towards the horizon than any of the versions seen on the market before,
And why sirio have updated their vector to have 1/4 wave radials with a 1/2wave upper monopole claiming improved low angle radiation,
Does that sound crazy to you Donald?
Can we honestly expect 2dbd from a 1/2wave + a sniff of radiation from the cone?
As Henry pointed out other factors can also contribute to the signal received at distance and we cannot ignore those possible effects as we adjust our antennas.
That's how it looks to me,
Id like to hear other peoples view if mine makes no sense to them,
thanks.