Jürg
This is very interesting assuming one can use this information to engineer
proton disintegration with minimal input energy.
To that end, it would seem necessary to know the resonance wavelengths in
question (or frequency of the 1/7th and 1/9th waves). From that information,
one could presumably try to maximally disrupt that resonance, possibly with a
beat wave.
Would this be the basic 53 MeV resonance you mention or is there a lower value
which works?
In the standard model, the scattering cross-section of the proton is around 1.5
fm (or 11 MeV) IIRC so there is a big gap there with available lasers.
Presumably Holmlid is doing this kind of disintegration with a laser. Holmlid
may have stumbled onto an effective wavelength which is not optimum. Who knows?
Perhaps his laser somehow stimulates a much shorter wavelength.
Jones
----------------
Jürg Wyttenbach wrote:
> The allowed torus resonances are 7 and 9 waves. The proton base state has 9
> waves.... The Holmlid proton split seen from the proton is: One out of 9
> proton waves starts the an orthognal 1/7 resonances what leaves behind a
> (2x2)x(2x2) wave structure without the biding glue of the 3D/4D waves. This
> wave pack (4x4) is repulsive as seen in 8-Be. The basic energy 53MeV for the
> split is delivered from the resonant 8H* --> 2 4-He (or 8-Be) conversion.
