So did you think a little bit about what I have written about Cassimer Invariance?
To bring back a recollection, Cassimer Invariance is the perpetual tendency of substringular phenomena interchanging eigenstates to maintain homotopy per instanton.
Here is some more knowledge that may help you to better understand what the directly prior deffinition means.: Phenomena that is substringular moves through Ultimon Flow in-between each instanton.
In ((2pi hbar-6hbar)+hbar Imaginary time) until an Imaginary Planck-Bar moment before instanton, phenomena goes through a duration that involves what I have described as the "space-hole" -- during which the Bases of Light appertaining to the ensuing instanton is organized. During this mentioned duration, substringular phenomena goes through relatively mild untying and retying of topology that is necessary for the changes that are necessary for substringular phenomena to not be frayed along with that phenomena that is frayed due to black-hole activity, as well as the mentioned untying and retying of topology just described is necessary in order for ensuing Gaussian Transformations to be spontaneously adjusted and allowed to happen. The condition that I have just described in terms of fascillitating Gaussian Translations and Gaussian Transformations to happen is necessary on account of the condition that space-time-fabric is not completely hermitian in terms of the multiplicit codifferentiation that surrounds any particular orbifold neighborhood. This may be related on account of the ansantz that not all orbifolds are Yau-Exact -- only mass and mass that is translated through a worm-hole is Yau-Exact. The condition that there is partially Yau-Exact and Chern-Simmons activity that sorrounds any substringular neighborhood that is completely Yau-Exact is evidence that shows the validity of the concept of the sentence that I typed just before this one. Wherever there is a mass, there is at least a certain degree of heat that is directly associated with that mass when one considers the duration in which any arbitrary mass that one could consider has vibrated in some sort of molecular manner over any measurable amount of time. Even if you could get a molecular arrangement to acheive absolute zero Kelvin over a certain arbitrary duration, there will always be a certain amount of electromagnetic and/or plain energy interaction that sorounds the general region in which an arbitary mass is existent in in any duration in which the said mass is able to molecularly vibrate. The condition that there is always a certain amount of partially Yau-Exact and Chern-Simmons differentiation that surrounds any arbitrary mass that is existent over any period in which any said mass is able to molecularly vibrate is proof that all Fourier Transfomations that are based on Yau-Exact orbifold translations are sorrounded to at least some extent by electromagnetic energy and/or plain energy. Since only Yau-Exact orbifold conditions are completely hermitian and non-spurious, both plain energy and electromagnetic energy always have a certain degree of Chern-Simmons behavior. Although electromagnetic-based energy is formed based on the hermitian motion of Fujikawa Coupling activity, the motion of plain energy and electromagnetic energy when scattered upon a mass always bears a certain degree of a lack of hermitian-based motion. This is why Fourier-based Gaussian Translations and Fourier-based Gaussian Transformations may only happen when there is a certain amount of retying of substringular activity. This retying can not happen during instanton on account of the need to maintain homotopy. Such retying can only happen right before the quaternionic-instanton-field-impulse-mode. Such a duration then is to happen during the duration in which the "space-hole" and the Bases of Light are organized. It is during the prior mentioned duration that the relatively Laplacian conditions that correspond the two general simultaneous gauge-metrics that the brief relatively mild retying of space-time-fabric is able to happen to the necessary extent so that the necessary norm-conditons of any particular region may be tweeked so that the said norm-conditions may contiue to codifferentiate with its surroundings. I am only able to describe so much at once. In time, you will get a clearer meaning as to what I am saying.
I will continue with the suspence later! God Bless You, and have a phenomenal day!
Sincerely,
Samuel David Roach.
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