In a polariton based hot spot, the electrons are part of a dipole where the
hole makes the electron a boson. Therefore *unlimited numbers *of electrons
can populate a hot spot.
The electrons combine with light and lose weight. They can weight as little
as 20 micro electron volts. These low mass polaritons will become entangled
and form a high temperature BEC.
When the Hot spot becomes mobile and forms a polariton bullet, these boson
connected electrons lose their holes and the electrons leave the hotspot
repelled by the coulomb force.. Only light remains and this light based
soliton spin structure may have been observed in many LENR experiments as
monopoles.
As I posted elsewhere, the magnetic field of this monopole comes from a
POINT in the center of a EMF current ring making it extremely concentrated
and very powerful. This energy focusing is what enables energy levels to
reach high enough power levels for nuclear disruption to occur.
On Thu, Nov 14, 2013 at 4:20 PM, <pagnu...@htdconnect.com> wrote:
> Robin van Spaandonk wrote:
> > In reply to Axil Axil's message of Wed, 13 Nov 2013 13:21:02 -0500:
> > Hi,
> > [snip]
> >>Light intensity at 10^^12 (watts/cm2) produces a strong Electric field at
> >>(10^^9) Volts/meter.
> > Over a distance of 1 nm (10 Angstrom) this is just 1 Volt.
> > [...]
>
> This is correct, but it only shows that a localized electron can only
> attain 1eV when crossing that gap unobstructed.
>
> For an electron, 1[eV] corresponds to an approximate momentum of
> 4 * 10^(-25) [N*sec] {'N' = Newton}
>
> However, if an electron is trapped in that field, i.e., the mean position
> of its wave function is fixed, for a time T instead of accelerating thru
> collision-free, it gains a momentum impulse
>
> = T[sec] * e[C] * 10^9[Volt/meter] {where 'e' = electron charge[Coulomb]}
> = T[sec] * (1.6^10^(-19)[C]) * 10^9 [N/C]
> = T * 1.6^10^(-10) [N*sec]
>
> So, in the latter case, the electron gains T*(10^14) times more momentum.
> ('T' measured in seconds.)
>
> Possibly, this happens when the electron collides with a particle of
> equal and opposite momentum.
>
> In quantum mechanics, a highly localized or oscillatory wave functions
> can posses high momentum (or kinetic energy) even when not moving much.
>
> Also, an electron is a fermion, so it really needs to be represented by
> a 4-component spinor in the Dirac equation. It can undergo more
> oscillation within the spinor.
>
> -- Lou Pagnucco
>
>
>
