Nice posts on the Rydberg effects, Axil. I like reading them. Please continue posting them. But, I am confused. Could you can help me understand these questions:
Rydberg hydrogen has a very loosely bound electron. How would these Rydberg electrons survive high temperature phonon collisions without the atom becoming ionized and as a result breaking up the condensate? With such large orbitals as Rydberg electrons occupy, how can such a phenomenon be considered inside a nickel lattice? The electron orbitals would extend greater than the nickel lattice spacing. Other condensates are possible, but why would you think these are Rydberg? While we know that the LENR appears to happen at the surface, and it also appears to require support from within the lattice (loading) - so it sounds like some kind of condensate effect is needed within the lattice. In the NanoSpire case, it is not clear how the H-O-H-O- crystals that form are Rydberg. What evidence supports this? They may be some kind of condensate, but not necessarily Rydberg. The large dipole moments you describe would certainly make it easy for the Rydberg atoms to couple to other atoms electronically and form a condensate from that coupling. However, I don't see how that strong dipole provides support for the charge evidence that you described from NanoSpire. Can you explain that a little more? *On Sun, Mar 18, 2012 at 11:03 PM, Axil Axil <[email protected]> wrote:* Rydberg matter and the leptonic monopol >> >> This post is third in the series on Rydberg matter which includes as >> follows: >> >> Cold Fusion Magic Dust >> >> Rydberg matter and cavitation >> >
