Part One of the 14th Session of Course 14

For every one-dimensional superstring of discrete energy permittivity that closes into a two-dimensional superstring of discrete energy permittivity, there is a two-dimensional superstring of discrete energy permittivity that opens into a one-dimensional superstring of discrete energy permittivity.  The directly prior eluded to Fujikawa Couplings and inverse Fujikawa Couplings are examples of Yakawa Couplings.  What a Fujikawa Coupling is is the bonding of the alterior ends of a one-dimensional superstring that initially functions as an operator of plain kinetic energy -- in so as to form a two-dimensional superstring that functions as an operational index of electromagnetic energy.  This is the case, when a discrete unit of plain kinetic energy that stems from the operational locus of an electron is pulled in a hermitian manner in so as to form a closed loop of integrated first-ordered point particles that is known of as a photon.  Whenever a photon is formed, there tends to be an equal and opposite reaction of a phontonic potential that loosens an initially closed-loop of a given arbitary locus that functions as a discrete unit of electromagnetic energy into an open strand that instead functions as a discrete unit of plain kinetic energy operational index.  So, whenever there is a Fujikawa Coupling, there tends to be an inverse Fujikawa Coupling.  The entity of the closing of one-dimensional superstrings into bosonic two-dimensional superstrings -- as well as the opening of two-dimensional superstrings that are closed loops into open strands that are here one-dimensional superstrings -- are zero-norm-state projections.  A zero-norm-state is a differentially isolated homotopic point commutator that acts as a first-ordered point particles that is not of a Campbell, Hausendorf, nor a Campbell/Hausendorf nature.  As such a first-ordered point particle is interconnected to other first-ordered point particles in a manner that is both of a somewhat abelian wave-tug/wave-pull Hamiltonian operation over a relatively transient duration, and, also here bearing no Campbell, Hausendorf, nor Campbell/Hausendorf homotopic differentiation -- in the directoral sway of its here considered holomorphic Hamiltonian gauge, such a tracing of the eluded to projection over the eluded to transient duration is said to function as what may be here termed of as a zero-norm-state projection.  The Clifford Expansion of the indirect leveraging of a Wick Action eigenstate upon the Poincaire field of a zero-norm-state projection -- that is proximal to the Poincaire field of an open strand of the directly corresponding first-ordered point particles -- that forms a given arbitary one-dimensional superstring of discrete plain kinetic energy that is here released from an electron, which is happening as the said electron is dropping an energy level, forms a cascading of Clifford Expansion in the eluded to locus of the mentioned substringular neighborhood of the said one-dimensional superstring that was released in so as to work to form a hermitian wave-tug/wave-pull that closes the eluded to open string in so as to form a bosonic closed string known of as a photon.  Such a hermitian closing of an open string acts as according to the Green Function.  The eluded to Poincaire field of such a Fujikawa Coupling acts as the euclidean-based holonomic substrate of the resultant binary Clifford Expansion that I have recently implied in this post.  I will continue with the suspense later!  Sincerely, Sam Roach.