Showing posts with label topological surface. Show all posts
Showing posts with label topological surface. Show all posts

Friday, January 13, 2023

Hermitian World-Sheet -- Smooth Homotopy

 When the mappable-tracing, as taken along the topological surface of a given arbitrary world-sheet, is hermitian, then it may be said, that the directly associated cohomology, is here to tend to bear a smooth homotopy. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SAM.

Thursday, February 17, 2022

Scalar Amplitude Of Wave-Tug -- Gauged-Action -- Angular Momentum

 The greater the scalar amplitude of wave-tug, that a directly corresponding respective gauged-action is to be physically applying, as this is here to be incurred upon the topological surface, of a Ward-Cauchy-Related structural manifold, as taken over the durational course of a directly corresponding Fourier-Related-Progression, the stronger that the directly associated scalar amplitude of the corroborative angular momentum, will therefore consequently tend to result in being exhibited, by the energy-related entity, of which is here to be engaged in its kinematic motion, in part, due to the fractal of pressure, of which is consequentially accomplished, by the innate utilization of such a general tense of a gauge-like action. SAMUEL DAVID ROACH. I WILL CONTINUE WITH THE SUSPENSE LATER! 

Friday, April 30, 2021

A Little As to When A Discrete Quantum Of Energy Is Gauge-Invariant

 In the general procedural course of "events," in which a given arbitrary discrete quantum of energy is to remain gauge-invariant, -- there is thereby to be the eminent resultant given arbitrary physical tendency, in which the directly associated kinematic flow of the respective local sequential series, in which one is here to be considering the "plucking" action of those directly applicable gauge-bosons, as these are here to be made Gliosis upon the topological surface of those directly corresponding second-order light-cone-gauge eigenstates, to where these said second-order eigenstates, that are here to work to make-up the holonomic substrate, of what basically amounts to being the proximal local presence of the wave-based nature of discrete energy impedance, -- will thence tend to occur in such a general manner, to where this inferred flow of a resultant formation of a set of Schwinger-Indices, that are here to externally propagate, in so as to interact with their infringed upon environment, in such a manner, to be able to form the forces of nature, to where this will therefore tend to work to form, in this particular genus of a case, a homeomorphic flow of force-related eigenstates, over a directly corresponding period of time. Sincerely, Samuel David Roach. (1989).

Wednesday, July 29, 2020

Inverted Concavity Of Cohesive Set Of Gravity Waves

If one were to theoretically invert the concavity of the cohesive set of gravity waves, that were initially to have been directly applied to the external topological surface of a given arbitrary Noether-based cohesive set of discrete energy quanta, -- this will often tend to help reverse the general tense of the correlative gravity, that was (is) here to be directly applied to the inferred physical entity of cohesive discrete energy quanta -- of such a particular case (Ex: Gravity -- Anti Gravity). To Be Continued! Sincerely, Samuel David Roach.

Friday, April 19, 2019

Relative Harmonics Of Fields

When harmonic Schwinger-Indices are to ripple along the topological surface, that is of a specific region of mini-stringular segmentation -- this will then tend to form a harmonic substringular field, at the proximal locus of the said region of mini-stringular segmentation.  Consequently, when anharmonic Schwinger-Indices are to ripple along the topological surface, that is of a specific region of mini-stringular segmentation -- this will then tend to form an anharmonic substringular field, at the proximal locus of the said region of mini-stringular segmentation.  I will continue with the suspense later! To Be Continued! Samuel David Roach.

Tuesday, August 7, 2018

Some Stuff As To Homeomorphic Field And The Beti Action

The Beti Action works to help at making a superstring of an orientable nature, in so that the said string may continue to differentiate in a Fourier-related manner -- in a Noether-based manner.
A superstring is to be made orientable during BRST by the Beti Action -- when the field that is here to exist in-between a given arbitrary superstring and its correlative counterstring, is said to be homeomorphic during a respective iteration of BRST.  A superstring is said to work to bear a homeomorphic field -- in-between itself and its correlative counterstring -- when the asymmetry that is to exist amongst the phenomenology that is of the dual-state that exists between the proximal local delineation of the partition-based discrepancies of the said superstring, & the proximal local delineation of the partition-based discrepancies of the said counterstring, -- is to be maintained with an even-functional-based pulse -- at the topological surface, that is Poincare to the region that is here to exist in-between the said superstring and its said counterstring.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Friday, May 14, 2010

Course 4 on The Globaly Distinguishable Vs. the Substringular, Session 8, Part 1

As told already, an electron's spin works to determine its magnetic field. This is because the magnetic field of an electron is normal to its electric field, and an electric field is based on the angular momentum of the given electron. Angular momentum is based on the directoral impetus of the electron in any series of locants, as implied before. In order for something to spin, the phenomenon has to go around. That's what spinning is. This means that the surface area of any object that spins must have radial translation after every discrete metric in which that object does indeed spin. Whenever something exists, it exists in some sort of space. Anything that exists in space is touching something, and at every spot in which it exists. Whenever there is touch, there is tangency. So, everything that exists involves tangency. The condition of tangency is normalcy. This is because wherever there's a tangency point, there is a norm vector. So, anything that exists has some sort of normalcy that is associated with whatever topological surface that you may wish to discuss. Normalcy may not always be associated with Real space, yet it is always associated with some sort of medium through which points or indices may be relayed or at least temporarily transferred. whenever radial motion happens, there is always at least a potential of spinning of either the object in radial motion or the indices that it translocates. Radial motion that differentiates homotopically through a metric always involves actual spinning. Let's say that you are a small point. You are on the surface of a smooth paraboloid. The paraboloid spins. Remember, you are touching the paraboloid. As the paraboloid spins, you spin with it. You are staying put on the relative spot of the paraboloid, now. So, you are in tact with a constantly differentiating norm vector that is kept in the sequential pattern of the spinning of the paraboloid. I will continue with the suspense of this session later. Until then, I hope that you are having a phenomenal day.
Catch you two!
Sincerely,
Samuel