I have been attempting to improve my understanding of nuclear reactions and 
have reached some interesting conclusions.  It has been known for many decades 
that the motion of a charged particle such as an electron or proton results in 
the emission of electromagnetic radiation.  The smooth non accelerated movement 
of this type of particle does not cause radiation to be emitted.  Only when the 
charge undergoes accelerated motion does energy spread out into open space.  
And, on occasions it is possible to have an accelerated charged particle that 
does not emit radiation if a proper structure exists that results in a balance 
by other particles.  An example of the later is when a ring of charged 
particles such as electrons are rotating in a circle in a direct current 
fashion.  Each individual electron would radiate energy as it is accelerated 
around the circle, but the contribution of the others results in a net balance 
of the radiated far field and we have a steady magnetic field.  I believe that 
a similar process occurs in electron orbital shapes and field distributions 
which results in a steady state non radiative condition.

The Mills theory seems to build upon this basic concept and arrives at some 
interesting conclusions.  Geometry and charge field motion might hold clues to 
LENR which we need to be open to.

My main reason for this thread is to uncover the emission of energy by the 
charge neutral particles associated with nuclear reactions.  At this point in 
my research I have been unsuccessful in locating a mechanism that allows 
neutrons and the like to emit energy associated with the binding of a nucleus.  
The only effect that I have observed thus far is through beta decay.  In this 
case I refer to either beta plus or minus decay and the neutrino type 
associated with each.  I am not aware of any reported radiated electromagnetic 
energy which usually occurs when a charged particle is accelerated.  I do 
expect to see a minor amount of radiation due to the release of the positron or 
electron at the moment that the neutron transforms into a proton or vice versa 
during the process since this would likely result in the acceleration of the 
charges.  The separation of the positive charge and the negative charge must 
show up in the far field as a pulse of radiated energy unless some form of 
magic field shape as suggested above occurs.

The strong force only acts over a very tiny distance so it should not be 
capable of allowing binding energy to escape into free space.  These conditions 
imply that there are most likely only two ways for binding energy to be freed 
during a nuclear reaction.  The first is by electromagnetic radiation as in 
gamma rays and the second is by ejection of  energetic particles such as 
neutrinos, protons, neutrons, electrons or etc.  Perhaps the list should 
include very high energy reactions as those associated with accelerators but I 
am most interested in the processes that occur in normal environments such as 
LENR devices.

Should the release of phonon energy just be considered another way of viewing 
the ejection of particles that are quickly retarded by the adjacent atoms?

Also, is the coupling of entangled nearby protons just another type of 
electromagnetic interaction?  I think that a process associated with this 
action might be the key reason that high energy gammas are not seen in LENR as 
the energy could be spread over a large number of protons instead of radiated.  
I have seen a remarkable difference in the behavior of near field versus far 
field electromagnetic devices.  Near field effects can extend for a relatively 
long distance, but still not result in significant radiation of energy into 
free space.

If anyone is aware of a mechanism that allows charge neutral particles to emit 
nuclear binding energy please direct me to the effect.  Thanks in advance.

Dave

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