When cohomologies bend in a hermitian-based manner that is of an assymmetric nature, this is an example of a topoloigical sway that is most exemplified by the nature of fermions. For instance, let us take into consideration electrons. Electrons are examples of fermions. Fermions are subatomic particles that bear a fractional spin. Even though electrons are comprised of both bosonic strings and fermionic strings -- the mass of an electron is composed of bosonic superstrings of discrete energy permittivity (vibrating hoops of discrete energy), and, the kinetic energy of electrons (that has not yet converted into electromagnetic energy) that works to comprise part of electrons, is composed of fermionic superstrings of discrete energy permittivity(vibrating strands of discrete energy. Electrons that are adjacent spin assymetrically -- when such covariant-based electrons are situated next to each other. Electrons are basically considered to be a pointal-based mass, and thus, the singularities that work to form the immediate Ward-Caucy boundaries of electrons, are of a Yau-Exact nature. Phenomenology that is of a Yau-Exact nature bear hermitian singularities. As electrons move, the superstrings that work to compose the holonomic substrate of the said electrons, work to form a physical memory of both the existence and the activity of the so-stated electrons -- in the form of a cohomological setting. Cohomologies are the integration of ghost-based indices. Ghost-Based Indices are the mapped-out physical stratum of world-sheets. World-Sheets are the projection of the trajectory of superstrings. As phenomenology moves over time, the topological stratum that works to form the correlative superstrings of discrete energy permittivity, bends -- as the inter-relation of the multiplicit covariant modes of the substringular are brought into the multivarious Yakawa Couplings, that both exist and occur over a sequential series of the iterations of group-related intantons. Yakawa Couplings are the touch, rub, and the curl of any one or more respective given arbitrary substringular phenomenon upon other substringular phenomena. A Gliossi-based Coupling is a Yakawa-based Coupling that is topologically of a direct physical contact. Since electrons bear a much higher charge density than protons (since electrons have the same charge as electrons, yet, with a much smaller volume than that of a proton), and, electrons are of the same like charge, electrons normally do not directly collide, and thus, electrons are a composition of a genus of orbifold eigenset that tends to not form a Gliossi-based contact upon other electrons. (The topology of electrons -- as these are directly the part of any given arbitrary electrons -- do not tend to strike the topology of other electrons, as these alterior mentioned phenomenology are, as well, directly the part of these respective latter mentioned given arbitrary electrons.) So, when electrons spin assymetrically towards other electrons, as these always tend to do, these tend to work to form a Yakawa-based Coupling that thence cause a cohomological genus of a hermitian-based bending -- as the ghost-based indices that work to comprise the so-eluded-to cohomologies are of a covariant-based mode, that may be either trivially or non-trivially isomorphic -- in an assymetric manner.
I will continue with the last part of this session later! To Be Continued! Sincerely, Sam Roach.
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