Part Three of Session 9 of Course 18

When one is dealing with first-ordered point particles in the substringular, one is dealing with condensed oscillation of mini-string or condensed oscillation of core-substringular-field-density -- that would here come together in a form that one may say acts like a  "ball of yarn" of the just-mentioned condensed oscillation -- in so as to form a given arbitrary degree of a compactification of the so-stated local multiplicitly torsioned core-field density, in so as to form one immediate eigenmember basis of what may be either termed of as a point commutator that would here work to form a superstring, or as a point commutator that would here work to form a superstringular counterpart.  So, when one is dealing with the extension of mini-stringular segments that are jutted-out from any given first-ordered point particle, that would here work to form a ground-based superstring of discrete energy permittivity -- besides those other given arbitrary mini-string segments that jut-out from the so-stated first-ordered point particle, in so as to work to interconnect the said point commutator to both the adjacent first-ordered point particles that work to form the same respective directly associated given arbitrary superstring, and, to the most adjacent first-ordered point particle of the directly corresponding counterstring of discrete energy permittiivity -- one is then  here working with only one of such jutted-out mini-stringular segments.  Yet, when one is, instead, dealing with the extension of mini-stringular segments that are jutted-out from any given arbitrary first-ordered point particle, that would here work to form a Fock-based superstringular counterpart of the wave-functionablitiy of discrete energy permittivity -- besides those other given arbitrary mini-string segments that jut-out form the so-stated first-ordered point particle, in so as to work to interconnect the said point commutator to both the adjacent first-ordered point partictles that work to form the same respective directly associated given arbitrary counterstring, and, to the most adjacent first-ordered point particle of the directly associated superstring of discrete energy permititivity  -- one is then here working with many of such jutted-out mini-stringular segments.  The orientation of any given arbitrary first-ordered point particle to its surroundings, where it is positioned in its neighborhood, and, the pointal localization of the said point -- when this is taken relative to its environment -- is the basis for a respective fractal of electric field.  The coordinates that make it a field are the single wave propagations that are extended from the just so-eluded-to substringular neighborhoods.  To Be Continued!  Sam.

Compactification and Yakawa Couplings, Course 5, Part 5, First Test

1) What is meant by that two masses differ in compactification?

2) What is meant by that two phenomenal discharges of equal total volume differ in compactification?

3) Describe how an umbrellas relate to compactification.

4) Describe how a quilt shows a lack of or a degree of compactification.

5) When is space an overt thing, and when is it nothing?

6) What makes differentiating space compactified?

7) How is a point particle like a ball of yarn?

8) Give the analogy I gave how all point particles are interconnected.

9) Thru what general transit are all point particles interconnected?

10) How are the spin and woll of the point particles related to this transit?

11) Spin and roll are related to what field phenomena?

12) The drive in a direction of a point is what and describes which part of "12?"

13) What is a Yakawa Coupling?