Often, when one is dealing with a Ward-Cauchy-related open-loop substringular phenomenology -- that is an open loop that is isotropically stable, -- one is to initially have two individually taken open substringular strands, that are to subsequently bend in a hermitian manner towards one another, in so as then to tie their initial fabric of the holonomic substrate of topological stratum, in so as to then to work to become an open-loop of substringular phenomenology. This is to happen, due to the cohesive activity of a correlative group-attractor -- that is to work to help at forming such a wave-tug, that is to both bring the initially stated open strands towards each other, plus to work at helping that activity of the hermitian bending of the two said open strands that is necessary in so as to work to form a resultant open-loop, as well as to help at working to initiate that interaction that is to happen between the dual state of the correlative mini-stringular segmentation that is to exist among each of such initial open strands, in so as to help at allowing for that Ward-Cauchy-related tying that is to happen, in so as to help at allowing such open strands to then to become one Ward-Cauchy-related substringular open-loop.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
Showing posts with label open strand. Show all posts
Showing posts with label open strand. Show all posts
Monday, January 8, 2018
Some More Knowledge As To Open-Loops
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samsphysicsworld
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group-attractor,
hermitian,
holonomic substrate,
isotropically stable,
open strand,
open-loop,
phenomenology,
substringular,
Ward-Cauchy
Monday, December 18, 2017
Homology Versus Cohomology
Here is the basic difference between what a homology is, versus what a cohomology is:
A homology is the physical memory as to the when, the where, and the how, that either an open substringular strand or an open substringular loop has differentiated, as a Hamiltonian eigenindex, over time. A cohomology is the physical memory as to the when, the where, and the how, that a closed substringular loop has differentiated, as a Hamiltonian eigenindex, over time. Such physical memories may be anywhere from being at a proximal locus, that is just external to the core-field-density of the superstring -- in other words, at the Ward-Cauchy-based field that is just external to the topological stratum of the substringular eigenindex, -- to being as a physical memory that may be extrapolated from the effect of such a respective strand or a loop, that has here to have just potentially differentiated through a Lagrangian that may be mapped-out, over a Fourier Transform that involves a sequential series of instantons.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
A homology is the physical memory as to the when, the where, and the how, that either an open substringular strand or an open substringular loop has differentiated, as a Hamiltonian eigenindex, over time. A cohomology is the physical memory as to the when, the where, and the how, that a closed substringular loop has differentiated, as a Hamiltonian eigenindex, over time. Such physical memories may be anywhere from being at a proximal locus, that is just external to the core-field-density of the superstring -- in other words, at the Ward-Cauchy-based field that is just external to the topological stratum of the substringular eigenindex, -- to being as a physical memory that may be extrapolated from the effect of such a respective strand or a loop, that has here to have just potentially differentiated through a Lagrangian that may be mapped-out, over a Fourier Transform that involves a sequential series of instantons.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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samsphysicsworld
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6:50 AM
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Labels:
closed loop,
cohomology,
eigenindex,
Fourier Transform,
Hamiltonian,
homology,
instantons,
Lagrangian,
open strand,
physical memory,
sequential series,
Ward-Cauchy
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