Refreshing People About Course Five

Hello. This is Sam Roach here. I am here to refresh you about the last course of string theory that I was in the process of putting into my physics blog. The course that I am referring to is Course Five on Compactification and Yakawa Couplings. You see, the whole idea of compactification in terms of the type of string theory that I have been writing about is the condition of mini-string -- of which is comprised of interconnected "beads" of second-ordered point particles -- going either from a state of being loosely fitted into the realm of the substringular region in which these exist to being tightly fitted into the realm in which these exist or are going from a state of being tightly fitted into the realm in which these exist to being loosely fitted into the realm in which these exist. The increasing tautness of the Caucy Ward boundary conditions of mini-string's holonomic region is a condition of compactification, while the increasing relaxation of the Caucy Ward boundary conditions of mini-string's holonomic region is a condition of decompactification. First-Ordered point particles have varying compactification levels of mini-string -- these bear more compactification of mini-string when existing as part of a superstring while these bear less compactification of mini-string when existing as a Fock related particle. Fock related particles may be either a norm state or a scattered point particle that does not form a direct Gliossi interconnection that would define it as a norm state. Second-Ordered and third-ordered point particles always bear the same level of compactification, since the fabric of the interboundedness of sub-mini-string may only disconnect in-between individual second-ordered point particles, and not otherwise, because of the lack of holonomic Hodge leverage that exists where the said sub-mini-string interconnects second-ordered point particles verses the fully compactified (except for the determinable sub-kernels) conditions that comprise the make-up of second and third-ordered point particles.
Yet, since mini-string may on occasion partially break homotopy when mini-strings enter a black-hole during the simultaneous occurrence of Cassimer Invariance which helps to consistently "heal" homotopy, mini-string and thus also superstrings are sometimes frayed in the course of the breaking of links of mini-string via black-holes. This is because superstrings are comprised of first-ordered point particles, and first-ordered point particles are comprised of relatively compactified mini-string. I hope that what I just wrote will help you to understand Course Five better in terms of compactification.
Yakawa Couplings are all about substringular associations. The condition of Gliossi touch, as well as the condition of touch that bears an unborne tangency of substringular phenomena, the condition of the substringular Gliossi rub a well as the condition of the rub of substringular phenomena that bears no borne tangency, as well as the condition of substringular Gliossi curl as well as the condition of the curl of substringular phenomena that bears no borne tangency, are conditions that are called Yakawa Couplings. One of the most prominent types of Yakawa Couplings is the Fujikawa Coupling, since this type of coupling is what describes how the kinetic energy of electrons converts into photons. Photons are discrete units of electromagnetic energy, and electromagnetic energy, besides the Higgs Action, is about the most important phenomena that allows reality to exist. Thank you for your time. I hope that this session will prepare you all for the continuation of Course Five. I will continue with the suspense later! Sam.