More As To Internal Quantum Well Boundaries

The case that I am discussing in both of today's posts, is if the Hamiltonian operation of the motion of the here respective given arbitrary orbifold eigenset -- forms such a cross between a fractal modulus and an elastic modulus, that is to strike a physical boundary that forms such a cross between a fractal modulus and an elastic modulus, to where most of the Hamiltonian pulsation of that orbifold egienset that is to here act in so as to strike the so-stated physical boundary -- is to be absorbed by the said boundary, yet, without resonating the selfsame mentioned boundary.  Just as the respective given arbitrary orbifold eigenset that I had mentioned in my last post (as to an orbifold eigenset that is reverberating in a semi-infinite quantum well), has struck one of the two ends of the so-eluded-to quantum well -- when this is taken at one of the individually taken ends -- the immediately prior loosened tense of its directly corresponding Majorana-Weyl-Covariant-Mode, is to then be spontaneously tightened to the extent that it was at, at the initially so-eluded-to instant under consideration, right before the so-stated orbifold eigenset was to accelerate from one end of the said semi-infinite quantum well to the other end of the selfsame quantum well.  This reiterative process is what helps the Noether Current of the said orbifold eigenset to slow back down to its initial rate of translation, at either of the two ends of the so-stated semi-infinite quantum well, as "well" as working to bring the velocity of the directly corresponding orbifold eigenset to go back down to its initial rate that I had eluded-to at the start of my last post -- in such a manner to where the directly corresponding orbifold eigenset is to accelerate from one end of the so-eluded-to Ward-Caucy boundary to the other, while then the selfsame said eigenset is to then be slowed back to its initial rate of propagation when it is to strike the other end of the said semi-infinite quantum well, -- while then the so-stated eigenset is to accelerate back to the rate of propagation that it had at the second so-mentioned end of the said Ward-Caucy end of the said quantum well, while then it is to be slowed back down to its initial rate of propagation that it had initially had, at that general Ward-Caucy-based end of the selfsame quantum well... to where this is to form an iterative process, that may be thought of as a reverberating eigenstate that is happening in a semi-infinite quantum well.
To Be Continued! Sincerely, Samuel Roach.