The evanescent wave

As experimentally demonstrated, there is an EMF power amplification factor
of up to 10 to the 15 power demonstrated by nanolenzes formed by nanowires
and nanoparticles. What EMF amplification that the Ni/H reactors produce is
undoubtedly higher.

The question is “how does such a concentration of power occur?”
An evanescent wave exits in the near-field of a reflecting surface with an
intensity that exhibits exponential decay with distance from the boundary
at which the wave was formed. Evanescent waves are a general property of
wave-equations, and can in principle occur in any context to which a
wave-equation applies. They are formed at the boundary between two media
with different wave motion properties, and are most intense within one
third of a wavelength from the surface of formation.

This is the reason why electric arching and dielectric boundaries are
important in LENR. EMF amplification involves solutions of Maxwell’s
equations and boundary conditions where imaginary solutions are manifest.

See

http://en.wikipedia.org/wiki/Evanescent_wave

Total internal reflection of light

In the context of Ni/H LENR+, the boundary between nickel and pressurized
hydrogen forms a boundary trap where the capacitive EMF(electrons)
accumulate because there is a Total internal reflection of this EMF at the
boundary of the metal hydrogen interface.

These electron waves accumulate and superimpose constructively. This EMF
wave function has no solution that transmits energy away from the boundary.

Mathematically, evanescent waves can be characterized by a wave vector
where one or more of the vector's components have an imaginary value.

This coupling between the hydrogen dielectric and the nickel is directly
analogous to the coupling between the primary and secondary coils of a
transformer, or between the two plates of a capacitor. Mathematically, the
process is the same as that of quantum tunneling, except with
electromagnetic waves instead of quantum-mechanical wavefunction.

This near surface interface boundary is the zone were electrons accumulate
by a power concentration factor of up to one trillion. It is this charge
concentration that produces coulomb barrier lowering in the boundary layer
where the evanescent wave forms.

http://en.wikipedia.org/wiki/Fano_resonance

Fano resonance is the mechanism that mixes the electron and light waveforms
together. The infrared radiation and dielectric oscillations of the
excitons are the two waveforms involved.

An exciton is a bound state of an electron and an electron hole which are
attracted to each other by the electrostatic Coulomb force.

The Fano resonance line-shape is due to interference between two scattering
amplitudes, one due to scattering within a continuum of states (the
background process) and the second due to an excitation of a discrete state
(the resonant process). The energy of the resonant state must lie in the
energy range of the continuum (background) states for the effect to occur.
Near the resonant energy, the background scattering amplitude typical
varies slowly with energy while the resonant scattering amplitude changes
both in magnitude and phase quickly. It is this variation that creates the
asymmetric profile.

The Fano resonance is how increased infrared stimulation of the micro
powder increases LENR activity. When DGT removes the hydrogen from their
reactor, the Fano resonance is destroyed.





On Sun, May 5, 2013 at 4:37 PM, <pagnu...@htdconnect.com> wrote:

> This is probably just a coincidence, but Ni-63 is used in krytons to make
> avalanche electrical breakdowns more predictable. See:
>
> Electric discharge in gases
> http://en.wikipedia.org/wiki/Electric_discharge_in_gases
>
> Krytron
> http://en.wikipedia.org/wiki/Krytron
>
> Lots of reported LENR results appear to involve arcing and
> dielectric/vacuum breakdown.
>
> Pardon if this has already been covered.
>
> -- Lou Pagnucco
>
> Jones Beene wrote:
> > Courtesy of SPECTRE ... err... make that the "new" Kurchatov  Institute
> >
> >
> > Possible Way To Industrial Production of Nickel-63 and the Prospects of
> > Its
> > Use
> >
> > Tsvetkov, et al. Research-Industrial Enterprise "BIAPOS", Moscow, Russia,
> > Formerly "Kurchatov Institute", Moscow, Russia
> >
> > Nickel-63 (a pure beta-emitter with a half-life of 100 years) is one of
> > the
> > most promising radionuclides that can be used in miniature autonomous
> > electric
> > power sources with a service life of above 30 years (nuclear batteries)
> > working on the betavoltaic effect. This effect is analogous to the
> > photoelectric
> > effect, with the difference that electron-hole pairs are produced in a
> > semiconductor
> > with p-n-transition under the action of beta-particles rather than
> optical
> > radiation.
> >
> > In addition to 63Ni, among all variety of radionuclides only tritium 3H
> > (half-life 12.3 years; Emax = 18.6 keV; Eav = 5.7 keV) and promethium
> > l47Pm
> > (half-life 2.62 years; Emax = 230 keV; Eav = 65 keV) can be considered as
> > candidates for the betavoltaic converter....
> >
> > All other beta-emitters are unsuitable for any of several reasons:
> >
> > 1)    accompanying gamma-radiation;
> > 2)    strong bremsstruhlung, which requires the use of radiation
> > protection;
> >
> >
> http://isotope.info/wp-content/uploads/2008/04/possible-way-to-industrial-pr
> > oduction-of-nickel-63-and-the-prospects-of-its-use.pdf
> >
> >
>
>
>

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