*Magnetic monopole beam * One of the amazing revelations that has come out of nanoplasmonic research and experimentation is the explanation of how the “dark mode” polariton soliton can produce a monopole magnetic beam. This amazing revelation is not theory; it is based on experimental results. But there is a theoretical explanation that goes along with the experimental data (10). The monopole magnetic beam becomes pronounced at polariton soliton (PS) intermediate energy levels since the Surface Plasmon Polariton (SPP) aligns all the spins of the polaritons inside the soliton to project out of the soliton from its center perpendicular to its direction of wave rotation.
The polariton has a spin of 2. The number of polaritons that can be absorbed into the soliton is not limited by the fermion exclusion principle. There is even an experimental micrograph that shows the soliton and the monopole beam coming out of it. This beam can project out to 100 microns away from the soliton. It is not only the spin of the polaritons that contribute to the power of the monopole beam but it is also the angular momentum of polariton rotation that multiplies the magnetic power of the beam. The vortex rotation rate acts like a train of gears where the microparticle (large gear) drives the angular momentum of the hydrogen Rydberg matter (small gear). In the most dramatic case, the 100 micron particle transfers angular momentum to a hydrogen Rydberg matter particle which is comprised of a large number of graphite like layered hexagonal disk assemblages with a diameter just a few atoms across. Each atomic layer receives angular momentum from the vortex on the surface of the micro particle and that vortex motion is transferred to the small atomic hexagonal disks comprising the Rydberg matter. The spin multiplier that comprises the monopole beam is proportional to the ratio between the circumference of the 100 micron particle to the circumference of the hydrogen Rydberg matter hexagonal disk. The monopole magnetic beam is a primary mechanism of catalytic action in LENR. The beam can reach out without being depleted and disrupt an indeterminate number of atomic sites. The experiments of J,C.Fisher can be explained by the action of this beam. http://www.markfisher.net/johnfisher/papers/Bigshower.pdf Energetic particle shower in the vapor from electrolysis This experiment informs us about the nature of the NAE. The experiment related in this article uses CR-39 particle detectors to show the production of energetic particles in the mobile NAE afloat in the vapor above an electrolytic LENR cell. This NAE has become mobile after it has become detached from its point of creation somewhere on the lattice of the electrodes within the cell as it moves upward in the vapor produced by the action of electrolysis and the heat that this electrode produces. This NAE produces hundreds of thousands of charged particles as it floats upward out of the cell. This reaction most probably produces alpha particles as the NAE raises on the vapor currents upward out of the cell. The analysis in the article finds that this NAE is a point source of these alpha particles by correlating the angles of the pits produced by the charged particles as the NAE rises. This behavior implies that the NAE supports a continuous and long lasting LENR process that proceeds over a considerable duration of time. This mobile type of NAE must decouple from its point of creation on the lattice of the electrode and floats on air currents like a particle of dust. The mesoscopic NAE must be massive in size to be so driven by molecules of air and water vapor. In this experiment, the monopole beam projects out of the center of the mobile soliton up to 100 microns as it floats upward. The mobile SPP soliton can produce LENR reactions at a distance or it can enter the CR-39 detector strips and initiate LENR reactions inside the structure of the detectors as John Fisher has reported in his experiments 10 - Half-solitons in a polariton quantum fluid behave like magnetic monopoles arxiv.org/ftp/arxiv/papers/1204/1204.3564.pdf
