The Next Part As To Session 3 Of Course 20

The condition that an electron will bear a tendency, of not only moving in as many spatial dimensions as the number of derivatives that it is changing in, yet, it will as well tend to work to bear holomorphic-based torsional eigenindices -- that will bend in as many spatial dimensions as the number of derivatives that it is changing in -- is a condition, that is akin to some of what may here be called of as Chan-Patton rules.  An electron exists as an orbifold eigenstate, of what may here be called of as an example of a Calabi-Yau space.  A Calabi-Yau space, tends to bear eigenstates -- that are Yau-Exact.  Consequently, an electron is one general classification of a Fourier-based spatial Hamiltonian operator, that tends to bend in a hermitian manner, in so long as it is moving in a Noether-based manner -- via its translation through what may here be the traversal of a Lagrangian that may exist from anywhere between six and ten spatial dimensions plus time.  Therefore, an electron, when moving in a Noether-based manner over time, will tend to bend in a hermitian manner -- by both moving in as many spatial dimensions as the number of derivatives that it is changing in, as well as such an orbifold eigenset (an electron) -- to here be working to bear holomorphic-based torsional eigenindices, that will as well tend to bend in as many spatial dimensions as the number of derivatives that it is changing in.  This tendency is in so long as the said electron, is to here be moving as a metrical-gauge-based Hamiltonian operator -- that tends to work to form a Rham-based cohomology.   I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.