*I know the resistive IR is much lower than the anomalous spectrum reported by Mills but if it causes the plasmons in the active material to resonate at a higher harmonic this would bring it much closer.*
The frequency of light in the hot spot is changed from infrared to the color blue in the range correspond to a blue spectral range with *hw* *≈ *3 *.*13 eV. On Mon, Jun 24, 2013 at 7:59 AM, Roarty, Francis X < [email protected]> wrote: > I know the resistive IR is much lower than the anomalous spectrum > reported by Mills but if it causes the plasmons in the active material to > resonate at a higher harmonic this would bring it much closer. I also > wonder about the applicability of spectrum measurements to the active > environment. I am pretty sure we see only an average of the spectrum from > the lattice and both sides of the active geometry - my posit is that > fractional Rydberg h result in lower frequency while Rydberg h results in > higher and that both can occur but the active geometry [cavity] favors > fractional formations so I would expect to see the hydrogen spectrum > broadened but more so on the low side. > > I also wonder if resonance can occur between fractional states where f/h2 > disassociates and recombines in synch with the plasmon resonance and that > photons emitted from these fractional state hydrogen is responsible for > the spectrum spread claimed by Mills. I had a passing notion that the 20% > metronome effect might even extend to favoring a specific pair of > fractional states to oscillate between- the spectrum anomaly is caused by > the slaved disassociations of fractional states and there may exist > favored pairs. Does anyone know how consistent the Mill's claimed spectrum > is? > Fran > > >
