Wednesday, April 30, 2014

Part Five of the Eleventh Session of Course 16

In the real world, superstrings that are bosonic  -- over one individual course of their substringular history, in which such discrete phenomena are closed loops -- are constantly vibrating as oscillating hoops, particularly over the course of instanton.  Likewise, in the real world, superstrings that are fermionic -- over one individual course of their substringular history, in which such discrete phenomena are open segments that are composed of first-ordered point particles that integrate as one relatively linear-based phenomena -- are constantly vibrating as oscillating strands, particularly over the course of instanton.  Certain laws work to govern the tendency and ability of superstrings of discrete energy permittivity to vibrate in the manner in which these do vibrate.  The vibration of any given arbitrary superstring -- over the course of an iteration of instanton -- is controlled by the condition of a directly corresponding harmonic-based oscillation.  All superstrings over the course of an individual iteration of instanton, are varied in the sway of their topological structure -- in both a stand-still consideration, and, also, in-between the multivarious gauge-metrics in which such superstrings act, in so as to behave as the discrete phenomena that these are, in order to be fundamental units of energy permttivity.  Such a topological sway always acts in so as to conform to an eigenbasis, for either any directly corresponding one-dimensional superstrings and for any directly corresponding two-dimensional superstrings.  Such an eigenbasis may be of either of an annharmonic nature -- when in terms of the delineation of its eigenvalues -- when in terms of one-dimensional superstrings, over the course of the correlative iteration of instanton, or, such an eigenbasis may be of a harmonic nature -- when in terms of the delineation of its eigenvalues -- when in terms of two-dimensional superstrings, again, over the course of the correlative iteration of instanton. The just eluded-to eigenvalues, in this case, work to describe the individual indices of the alteration of the directly corresponding Ward-Caucy derivatives, that works to describe the flow of the eluded-to Ward-Caucy-Plane -- in either a non-metrical and/or in a metrical-based manner.  The changes in Ward-Caucy denotations in the said superstrings work to describe harmonic oscillation eigenvalues, while, the different curved contours of any given arbitrary substringular space work to describe harmonic oscillation eigenspaces.  The different conditions that work to allow for superstrings to harmonically oscillate over a sequential series of group instanton  -- in a relatively hermitian manner -- are the gist of Chan-Patton factors.  This is why perturbations in the flow of a set of superstrings by a tachyonic flow, over time, is a key relation that works to temporarily break Chan-Patton factors. I will continue with the suspense later!
To Be Continued!  Sincerely, Samuel Roach.

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