First-Ordered-Point-Particles comprise superstrings.
Second-Ordered-Point-Particles comprise the mini-string that "balls-up" to form first-ordered-point-particles, while these second-ordered particles also form all mini-string that forms substringular fields.
Third-Ordered-Point-Particles only exist so as to form the composition of second-ordered-point-particles.
Sub-Mini-String binds together third-ordered-point-particles as well as interconnecting the said second-ordered-point-particles.
Just as mini-string forms all substringular fields -- and also considering the condition that second-ordered-point-particles are two orders lower in diameter than superstrings -- sub-mini-string is what binds the mentioned second-ordered-point-particles.
Catch You Two,
Samuel David Roach.
Showing posts with label First-Ordered-Point-Particles. Show all posts
Showing posts with label First-Ordered-Point-Particles. Show all posts
Monday, December 12, 2011
Thursday, October 14, 2010
Course 5, Session 15, Part One
Well hello again world, this is Samuel David Roach here! How are you doing?!
So, get your mind into overdrive, and savor some of the thoughts that I am about to present to you.
Initially, let's backtrack to where I left off last time. First-Ordered point particles in the scenario that I had recently left you at in the second part of the fourteenth session of course 5. After the said first-ordered point particles go through the middle of the Main Heterotic String fabric that binds one set of parallel universes to the set of parallel universes that are positionally oriented to the initial set according to the sequential basis of: 1 to 2; 2 to 3; or 3 to 2;, these said point particles go up the Main Heterotic String Fabric of the adjacent set of parallel universes. Once these said point particles are back to the world-tube of the adjacent set of parallel universes, these travel around the succeeding world-tube with the said tori-sector-range that one is dealing with until these said point particles reach the preceding locus of the positionally antiholomorphic spot where the tori-sector-range that forms a Basis of Light there for that set of parallel universes will localize at the succeeding sub-metric in which that Basis of Light there will form soon before the next instanton. The said first-ordered point particles will then enter the Fabric of the Main Heterotic String that is directly norm to antiholomoriphically positional there in order to go "down, across, and up" to the succeeding set of parallel universes according to the sequential basis of: 2 to 3; 3 to 2; or 2 to 1;, in the same manner as before, except involving a sub-metric Imaginary Fourier group gauge-metric that involves an interaction of different tenses of sets of pararllel universes. Upon entering to the just described sets of parallel universes, the said point particles differentiate as before to complete the (n-1) entery into other sets of parallel universes that partake of the total ((n-1), (n+1)) redistributions that involve the interactions of first-ordered point particles with the alterior world-tubes that such point particles normally do not kinematically differentiate in during any particular instanton. Later, I will explain the prior mentioned "(n+1)" redistribution mode that I am trying to teach here under the example that I arbitrarily name as an "(n+1)" mode, as well as why I define these modes as such. Once you understand what I mean by these modes, it will become clear as to why first-ordered point particles generally only kinematically differentiate in a Fourier manner in their set of parallel universes. I will bring these concepts into fruition in the minds of those who have strong right and left brain minds once I have fully discussed courses 5 and 6 to completion. The second part of this session will thus be larger than this first one.
I will continue with the suspense later. Until then, you have a phenomenal day! Sincerely, Sam.
So, get your mind into overdrive, and savor some of the thoughts that I am about to present to you.
Initially, let's backtrack to where I left off last time. First-Ordered point particles in the scenario that I had recently left you at in the second part of the fourteenth session of course 5. After the said first-ordered point particles go through the middle of the Main Heterotic String fabric that binds one set of parallel universes to the set of parallel universes that are positionally oriented to the initial set according to the sequential basis of: 1 to 2; 2 to 3; or 3 to 2;, these said point particles go up the Main Heterotic String Fabric of the adjacent set of parallel universes. Once these said point particles are back to the world-tube of the adjacent set of parallel universes, these travel around the succeeding world-tube with the said tori-sector-range that one is dealing with until these said point particles reach the preceding locus of the positionally antiholomorphic spot where the tori-sector-range that forms a Basis of Light there for that set of parallel universes will localize at the succeeding sub-metric in which that Basis of Light there will form soon before the next instanton. The said first-ordered point particles will then enter the Fabric of the Main Heterotic String that is directly norm to antiholomoriphically positional there in order to go "down, across, and up" to the succeeding set of parallel universes according to the sequential basis of: 2 to 3; 3 to 2; or 2 to 1;, in the same manner as before, except involving a sub-metric Imaginary Fourier group gauge-metric that involves an interaction of different tenses of sets of pararllel universes. Upon entering to the just described sets of parallel universes, the said point particles differentiate as before to complete the (n-1) entery into other sets of parallel universes that partake of the total ((n-1), (n+1)) redistributions that involve the interactions of first-ordered point particles with the alterior world-tubes that such point particles normally do not kinematically differentiate in during any particular instanton. Later, I will explain the prior mentioned "(n+1)" redistribution mode that I am trying to teach here under the example that I arbitrarily name as an "(n+1)" mode, as well as why I define these modes as such. Once you understand what I mean by these modes, it will become clear as to why first-ordered point particles generally only kinematically differentiate in a Fourier manner in their set of parallel universes. I will bring these concepts into fruition in the minds of those who have strong right and left brain minds once I have fully discussed courses 5 and 6 to completion. The second part of this session will thus be larger than this first one.
I will continue with the suspense later. Until then, you have a phenomenal day! Sincerely, Sam.
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