Plasmon entangles with heat when their energy levels are equal. This is what produces plasmon polaritons. Ultra dense deuterium is not needed to host the polariton condensate. What is needed to create this condensate is a high level of polariton creation. Ultra dense deuterium greatly facilitates this increase in polariton density because of the superconductive nature of this ultras dense material's superconductive surface which maximizes the lifespan of the polaritons. But a high polariton production rate can get to the critical polariton density needed for a polariton condensate to form. When this condensation condition is reached, then the heat production begins.
The micro cavities in the mesh provides the amplification mechanism needed to help for polaritons formation, since the mixing of photons and plasmons is maximized by having a longer time to reach energy equilibrium. There is also a optimum mesh size that aids in the resonance between the plasmons, and phonton energy that leads to polariton formation. This mesh concept standardizes and optimizes the cavity based polariton formation process. https://en.wikipedia.org/wiki/Surface_plasmon_polariton A grating coupler matches the wave vectors by increasing the parallel wave vector component by an amount related to the grating period (Figure 2). This method, while less frequently utilized, is critical to the theoretical understanding of the effect of *surface roughness <https://en.wikipedia.org/wiki/Surface_roughness>*. Moreover, simple isolated surface defects such as a groove, a slit or a corrugation on an otherwise planar surface provides a mechanism by which *free-space radiation and SPs can exchange energy and hence couple*. On Thu, Jul 25, 2019 at 4:16 PM Jones Beene <jone...@pacbell.net> wrote: > Axil Axil wrote: > > > The palladium coating must serve only to provide a better surface > plasmon performance profile than does nickel. > > Not exactly the "only" purpose but certainly the Mizuno breakthrough does > appear to have a plasmon methodology for thermal gain using dense > deuterium. Palladium is the co-catalyst for densification. This is the part > Mills perhaps got right - you need many catalysts to maximized shrinkage > and nickel alone will not do it alone. > > Palladium has narrow optical properties; but primarily, it is the primo > spillover catalyst, which would be responsible - acting in sequence with > nickel to provide 6-7 different Rydberg levels for forming dense deuterium > from D2 gas. Perhaps it is a cascade - all the way down to the Dirac level. > > A plasmon methodology would also explain why "Type A" Pd alloy is or > should be used. > > As I recall, the silver content is surprisingly high in Type A - > something like 25% of the alloy. Silver is extraordinarily photoactive > (which is why compounds of silver were used in photography in the days > before digital). In a plasmon only context - silver makes more sense than > palladium. > > BTW if plasmons are the operative mechanism then much better results will > be had by dispensing with the heater coil and finding the proper LEDs to > radiate only the exact frequency which is needed (through a window)... > which would mean the red photons at ~590 nm in most cases. > > As it is now - heat from resistance wire does have a strong red line but > also 90% of the energy is in frequencies not needed for plasmons - and > wasted. Mizuno could bump the COP way up with photon irradiation at the > plasmon frequency. > > It all fits together... on paper :-) > > > > >
