On Wed, Jul 15, 2015 at 3:24 PM, <[email protected]> wrote:

I realize what you meant, but during normal decay reactions, the energy is
> not shared with an ensemble of electrons, so why would this case be special?
>

I'm not really sure.  There's just enough of doubt on my part about the
applicability of known behavior to this specific situation that I don't
write off the possibility.

Here are some potential explanations:

   - In the case of a short-lived nuclear transition yielding a gamma that
   occurs from the rearranging of nucleons, the nucleons reside in a field of
   strong positive charge, despite the presence of an electron cloud (I
   suspect).  Perhaps the charge density has to be negative or strongly
   negative for a gamma-yielding transition to short-circuit to nearby
   electrons.

   - Maybe when it comes to gamma-yielding transitions, there is more
   natural activity than we think there is, and a lot of the transitions are
   short-circuited in the proposed manner, leading to heat rather than
   gammas.  As observers outside of the system, we see only those gammas that
   escape for some reason.

   - Maybe there is a qualitative a difference between metastable
   transitions, which take a while to occur, and that of an extremely
   short-lived resonance like a [dd]* pair.  The faster the transition, the
   more likely it is to short-circuit.  Because we generally study dd fusions
   in a plasma system, this skews the data we have to work with, because there
   are few electrons nearby.  (In cases where a dd fusion occurs during
   thin-foil ion bombardment, there is an anomalous screening effect.)

   - Perhaps the circumstances of the production of the alphas are a little
   different than simple fusion in the vicinity of lattice sites; for example,
   if there is electric arcing which is drawing the precursors near one
   another (which may or may not be d+d), the arc in conjunction with the
   electron cloud may provide a different environment than is witnessed in
   other contexts.

Eric

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