Jones—

You mention a dense hydrogen isomer.  What do you mean?  Hydrogen metal with 
all nuclei having the same spin direction?  Are you suggesting   a dense 
molecular hydrogen?

BOB COOK

From: Jones Beene
Sent: Wednesday, March 1, 2017 12:35 PM
To: Vortex List
Subject: [Vo]:Mayer, Mills and hopping neutrons


Interesting factoids which link Mayer to Mills via the Compton wavelength and 
Rydberg energy and dark matter. Ref: "Electromagnetic Composites at the Compton 
Scale" Mayer and Reitz. This has not been mentioned before, as far as I know, 
but combining some numbers we see: 
136 * 27.2 eV = 3,699.2 eV (3.7 keV)
Contrast that with Meulenberg's
511 keV/137 = 3.7 keV 
I'll come back to these numbers at the end but first, can we bury the neutron? 
When one retreats to fundamental observations in Nickel-hydrogen thermal 
anomalies, going back 27 years, there is almost certainly no neutron 
involvement (either real, virtual, hopping, cold, or ultra low momentum)... 
since after very long overunity runs (over one year for Thermacore) there was 
zero neutron activation in the apparatus. 
Neutron activation is easy to detect, even if few neutrons are emitted; 
therefore, when there is absolutely no activation, why not acknowledge the fact 
and drop the notion like hot potash? If we begin with the premise of zero 
neutrons and no beta decay, an intriguing possibility for thermal gain from 
fast electrons is still justified... and yes, it still looks like beta decay to 
the observer, due to the fast electron. Plus, the weak force may be involved in 
a unique non-nuclear way as a continuum in an electroweak unified force range.

But here it is, a secret hidden in plain view - the k-shell... or more 
precisely, the k-shell meets dense hydrogen with a common denominator of 3.7 
keV.
If the gain in LENR can be shown to involve k-shell disruption of a reactant - 
either lattice metals or especially potassium, then we have crossed a 
significant conceptual hurdle. The reactant has a small repository for two fast 
orbital electrons, yet with no apparent way to dislodge them... until dense 
hydrogen comes along. And this makes the gain chemical in nature - not nuclear. 
This is desirable, even if we need to call it "supra-chemical" to distinguish 
it from valence chemistry. 
Recently, a strong and narrow radiation band of around 3.56 keV attracted 
unprecedented attention in the international astrophysics and particle physics 
communities (and Vortex). The dark matter identity is still not settled but 
potassium k-shell fluorescence is a candidate, as is dense hydrogen, new 
neutrinos and a few others. We have several threads in the archives discussing 
the connection to dense hydrogen to dark matter. Can 3.56 keV emission line be 
reconciled with 3.7 keV of Mayer? 
Maybe. Gravitational red-shift is possible. Anyway, according to Mayer, the 
electron is bound to the proton at 3.7 keV in a dense hydrogen isomer. He comes 
across this value differently from Mills. This energy value comes from Mayer's 
model of Schrodinger/Compton... and makes as much sense as Mills progressive 
drop since it fits the K-shell electrodynamics of transition metals such as 
nickel and palladium and especially - potassium k-shell fluorescence. We have a 
known 3.7 keV line which means the location of gain is the potash inner 
orbital, a detail that any medieval alchemist would have suspected.

Consider the particle described as the tresino of Mayer or hydrino-hydride of 
Mills, which has a negative charge and a tight radius. The critical issue is 
precisely when the dense hydrogen atom picks up and sheds the extra electron 
... and/or is that electron a k-shell electron of a host atom. 

In a metal lattice, dense hydrogen can approach a nucleus but cannot fuse. 
Instead it may encounter an electroweak force which otherwise promotes beta 
decay but in this case is attenuated but can break up dense hydrogen and 
accelerate an electron out as if there had been a beta decay. But in fact, 
there was no real beta decay and nothing changed drastically in the host 
nucleus itself.
This dense-hydrogen identity is becoming a tidy little package now, merging 
Meyer, Mills and Meulenberg at 3.7 keV. Of course, it could all be coincidental.

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