Tense Of Symmetry

A diffeomorphic phenomenon is most associated with a field -- that works to bear an isomorphic symmetry, that is to be taken in a Laplacian-related manner.  Whereas -- a homeomorphic  phenomenon is most associated with a field, --  that works to bear an isomorphic symmetry, that is, instead, to be taken in a Fourier-related manner.  To Be Continued!  Sincerely, Sam.

The Test Questions To the First Test of Course 14, Session 7

1)  What is a veilbien?

2)  What is a tetrad?

3)  What is a trivial isomorphism?

4)  What is a nontrivial isomorphism?

5)  What is a cyclic permutation?

6)  What is gauge-invariance?

7)  What is gauge-transformation?

8)  What is topological invariance?

9)  What is topological transformation?

10)  How do points flow through the Ultimon during Ultimon Flow?

An Aside As To The Light-Cone-Gauge

The flow here mentioned forms a Dirac-Based cone-like perturbation that has an increase in Hodge-Volume that is here an example of what I meant by a Clifford Expansion.  (Reminder).
The said curves are non-trivially isometric if folded in the directoralization of the given Real-Reimmenian holomorphic Laplacian-Lagrangian, since inversely delineated hyperbollic curves bear assymptotic distributions that map-out an inverse chirality that thus does not overlap directly in terms of topological allignment -- in the course of the mentioned sub-Laplacian distribution frameworks that one would be dealing with here.
If, on the other hand, one were to map out  the hyperbollic curves that appertain to the holonomic basis of the mentioned expanding sub-Fourier Clifford-field partial thru a Njenhuis norm-to-holomorphic topological-based sway, in such a manner so that the connection at the Fadeev-Popov-Trace is maintained as a conipoint of the associated coniaxial, then, the isomorphism of the said curves would be trivial in terms of the chirality of the mentioned 2-d superstring's light-cone-gauge.  This is based on the Ward-Caucy delineations that may be determined by the corresponding proximal effects of the here given arbitrary Lorentz-Four-Contraction field index that acts upon the specific direct neighborhood of the said given 2-d superstring.
  When one is dealing with the Clifford-expansion that relates to the sub-metrics that are similar but different during specific given examples that relate to the light-cone-gauge that is involved with 1-d superstrings, the main difference here is that one is then relating to a flat partial field that may be mapped out in this case in a purely Minkowski manner -- instead of dealing with a volume-based partial field that may be mapped out in the prior described case in a Hilbert manner.
I will get back to the session of Course 10 that I left out a while ago in one of my next posts.
I will continue with the suspence later!  Sincerely, Samuel David Roach.  

A Little Bit About Changes In Symmetry

A superstring that is orientable differentiates kinematically via Noether Flow. A superstring that is not orientable differentiates kinematically via a tachyonic flow. A superstring is orientable when the substringular field eigenstates that are first-ordered and supplementally norm between a given superstring and its corresponding counterstring are trivially isomorpphic in terms of the connections in-between the associated superstring and its corresponding counterstring as caused by the Bette Action, and if the delineatory amplitudes of these said connections have the same scalar distribution when considering all of the said first-ordered substringular field eigenstates, even if the Hodge distribution among the said field eigenstates is not homogeneous and therefore not integrably hermitian during the Laplacian condition of the given instanton in which the associated Bette Action is occurring through its described gauge-metric. If a superstring is not orientable during the Bette Action, the superstring described will attempt to become orientable during the subsequent gauge-metric of a given Regge Action via a Regge Slope that "totters" the associated superstring in an attempt to obtain the multiplicit trivial isomorphism and a common homogeneous and delineatory amplitude that bears a supplementally norm abelian nature that retains the Noether Condition of the said superstring's wave-tug. (This is via a simultaneous internal push-and pull that is exterially projected along the ultimon.) If a superstring is strill orientable during the Regge Action, then the associated superstring becomes tachyonic. This is an example of how a lack of substringular super-symmetry may effect the differential operation of that superstring over a simple Laplacian Transformationm which, if such a condition is integrable over a sequential series of iterations that is non-trivial gauge-metric-wise, will form a Fourier Transformation that involves a superstring that is tachyonic and thereby perturbative relative to its general condition of Noether Flow. Such a perturbation effects the matrix of the delineatory index of the involved orbifolds that are directly effected by this tachyonic multiplicitly integrable distribution. Since the anharmonic multiplicit redistribution of a kinematically unorientable superstring flows differently then the surrounding Noether Conditions, and Noether Conditions are the kinematic delineatory means of maintaining the norm conditions that allow for a sustained covariant Gaussian Symmetry, the Fourier Transformaion involved with a tachyonic flow will produce change in Gaussian Symmetry either via a regular Gaussian Transformation or via a gauge-transformation, the latter of which is the substringular cause of entropy.                


Sincerely, Samuel David Roach. samsphysicsworld@blogspot.com.                                                        

A Little Bit More Explaination As To The Construction of the World-Tubes

Well hello again world, this is Sam Roach here!  I hope that you are enjoying my physics writings!
The "world-tubes" that involve forward moving time are interconnected via the Lagrangian-based majorized annuli that connect the adjacent of such tubes in an interior directed sense. Such annuli are existent at the interior center of such "world-tubes."
The "world-tubes" that involve backward moving time are interconnected via the annuli that connect the adjacent of such tubes in an interior directed sense.  Such annuli are existent at the interior center of such "world-tubes." 
The "world-tubes" of the substringular encoders are interconnected with the world-tubes of superstrings -- one of such encoder tubes per two forward moving time involved tubes that correspond to one set of parallel universes, and one of such encoder tubes per two backward moving time involved tubes that correspond to one set of parallel universes.  A substringular encoder of forward moving time has the same general Laplacian shape as the corresponding encoder of backward moving time, except that the isomoriphism of two of such encoders is in a reverse directoralization.  The substringular encoders are interconnected relatively just below the center of where the two "world-tubes" meet.  There is an open region between where a substringular encoder is and the spread of where the mini-string that these tie into are to interconnect the corresponding superstrings and their associated Planck phenomenon related phenomena.  This process makes a suppositional set of three tubes act as one tube, in a sense.
  The substringular encoders are relatively just above the relative top of the Fabric of the main initiating positions of what I call a Main Heterotic String.  So, forward and backward moving space-time fabric bear opposite tenses of what is relative "up" in the substringular fabric and of what is relative "down" in the substringular fabric if one where to observe such substringular fabric from its exterior.  So, there is more than one of such six-pointed-star majorized regions of the Main Heterotic Fabric that open up to allow for the flow of superstringular related phenomena per set of parallel universes.
When phenomena initially flows into the Main Heterotic String Fabric, such phenomena flows into the region where the substringular encoders were, since the encoders are relatively "below" where regular space-time-fabric as we know it exists, while then entering the prior named Fabric.  This would involve 8*10^(98) superstings for each universe of one main kinematically-based tori-sector-range and 8*10^(98) Planck phenomenon related phenomena for each universe of one main kinematically-based tori-sector-range in the forward moving time section of the Ultimon in-between instantons, and 8*10^(98) superstrings for each universe of one main kinematically-based tori-sector-range for each universe of one main kinematically-based tori-sector-range and 8*10^(98) Planck phenomenon related phenomena for each universe of one main kinematically-based tori-sector-range in the backward moving time section of the Ultimon in-between instantons.
The annuli that interbinds two forward or two backward moving time related world-tubes is larger than the annuli that interbinds such world-tubes of the arbitrarily other two sets of parallel universes.
If the time directed tense of superstrings is to go the other way, then some of the superstrings of one substringular encoder that involves one tense of time will ebb mini-string so as to allow certain of its corresponding superstrings to travel relatively "down" to the space-time-fabric of the opposite directed tense of time until a space-time-coordination is established, while then the forward moving space-time direction will become re-established from that point.  I will continue by providing the test questions for the last test of Cousrse 5 later.  You have a phenomenal day!  Sincerely, Sam.