Showing posts with label stronger. Show all posts
Showing posts with label stronger. Show all posts

Tuesday, December 27, 2022

Anti Gravitational Force -- Depth Of Kahler-Based Quotients

 As a general tendency; It may often occur -- that the stronger the incursion of an anti gravitational force, as it is to be imparted upon a given arbitrary correlative Noether-Based mass-bearing Hamiltonian Operator, the deeper that its directly associated Kahler-Based quotient, may often tend to become. SINCERELY, SAMUEL DAVID ROACH. (PHS -- 1989).

Wednesday, August 24, 2022

Relatively Strong Majorana-Weyl-Invariant-Mode -- Relatively Strong Drive In A Direction

 The stronger the Majorana-Weyl-Invariant-Mode, the stronger that the drive in a direction will often consequently tend to be, of which is here to be of the directly associated respective Hamiltonian Operator, that is here to be exhibiting such an inferred tense of a relatively strong Majorana-Weyl-Invariant-Mode.

'TILL NEXT TIME, AT THIS BLOG CITE! TO BE CONTINUED! SINCERELY, SAM ROACH.

Tuesday, March 1, 2022

Stronger Harmonic Superstring-Related Dispersion -- More Intensified Hermitian Cohomology -- More Isotropically Stable Electromotive Current

 The stronger that the harmonic superstring-related dispersion is to be -- The more intensified that the consequentially formed hermitian cohomology is to tend to be -- To, where; The more isotropically stable that the consequentially formed resultant electromotive current, is therefore to tend to end-up becoming. TO BE CONTINUED! SAMUEL. 

Saturday, February 19, 2022

Strong Structural Modulus

 The “stronger” that the structural modulus is to be, for a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta, the greater the scalar amplitude of a net gauged-action, that it will tend to consequently be able to potentially withstand. TO BE CONTINUED! SINCERELY, SAMUEL.

Friday, October 8, 2021

Density Of Hamiltonian Operator -- Recursively Smooth Ricci Flow

 The denser of a proximal local covariant transferred region, that a given arbitrary kinematic Hamiltonian Operator is to bear, at the covariant successive loci, through which such an inferred overall energy of a system is to be sequentially transferred through, over time, to where such a respective Hamiltonian Operator, is here to be exhibiting the display of a radially transferred recursively smooth Ricci Flow, over the course of such an insinuated given arbitrary proscribed Fourier Transformation, the stronger of a tense of isotropic stability (group action), that such a said respective given arbitrary Hamiltonian Operator, will consequently tend to result in working to exemplify. TO BE CONTNINUED! SINCERELY, SAMUEL.