Other Neat Ideas 5

 When a discrete physical charge is to be incurred, upon an eminently associated Hamiltonian Topological Manifold, that is here to be in the general process, of spontaneously becoming enhanced into a heightened tense, of a compacted/de-compacted dimensional exemplification of spatial expression, that the consequential charge impartation, that is henceforth to be spontaneously exhibited, by this implicitly enhanced eigenstate of chiral-based magnetism, will thereupon ( or would it?) tend to bear a corroboratively demonstrative Imaginary pulsation, that is here to often tend to bear a tense of upholding an interdependent vanguard, upon both the immediate past & the immediate future, Lagrangian-Based interface of the traceable path integral, that it is here to be trekking upon.

Please comment on this one. I believe I have reason to suspect what I am implying by imagining this!!!PHS1989.

Imaginary magnetic adhesion, may often tend to pull one eminently into the future. Whereas; Imaginary magnetic repulsion, may often tend to pull one eminently into the past. So; If a given arbitrary transportation-based device, were to bear the likings of a general flow of Imaginary charge, that was to recursively, after the implementation of a recursively incurred application of Real Riemann-Related charge, that was to pejoratively include — if not in even in a majoritarian manner — in between each of such recursive flows of Imaginary Charge — go from a tense of Imaginary magnetic adhesion to a tense of Imaginary magnetic repulsion back into a tense of Imaginary magnetic adhesion… and so forth; — that such a general physical operation, may, at times, work to facilitate a torque-like energy efficiency in the implicit aerodynamic craft, for at least a relatively decent proscribed duration, and this may sometimes be a tactic to be utilized, if and when the theoretical ideal lack of net mass loss to the ship’s energy supply is not kept ample, due to things I won’t say here. 

Physically expressed Nijenhuis frequencies, of which are here to be demonstrably exhibited by the general venue of kinematically propagated spatial disturbances, may often tend to be eminently corroborative, to the general likings of the physical operation, of zero-pole-based Fourier-Related Transformations, as these are here to be denotable as being kinetically transferred, when in lieu of the potentially likely case scenario, in which one is here to be considering the loop-like manner by which time is often to be expressible as, since time can move both forward and/or backward, since it's not purely linear. This is primordially eminent, when one is to be in the general position of time traveling. 

The dimensional compactification of a Hamiltonian Topological Manifold, will often tend to be eminently corroborative, with Imaginary magnetic adhesion. Whereas; The dimensional de-compactification of a Hamiltonian Topological Manifold, will often tend to be eminently corroborative, with Imaginary magnetic repulsion. 

The dimensional compactification of a Hamiltonian Topological Manifold, will often tend to be eminently corroborative, with jumping into the future. Whereas; The dimensional de-compactification of a Hamiltonian Topological Manifold, will often tend to be eminently corroborative, with jumping into the past. Again; Dimensional compactification, is eminently corroborative, with a spatial situation, in which there are less spatial dimensions involved, yet to where, everything else is otherwise analogous. Furthermore; Dimensional de-compactification, is eminently corroborative, with a spatial situation, in which there are more spatial dimensions involved, yet to where, everything else is otherwise analogous. This is NOT to be confused with Lorentz-Four-Contraction-Related activity, in which there is, in this latter just mentioned case scenario, there is to be an attenuation in the scalar amplitude, of one or more metric-related spatial parameters, of which are here to be denoted to the dimensional configuration, of the implicit team of energy. 

First off; I wanted to recap something, that I’ll admit I haven’t made clear enough. The Betti Number, is an Imaginary Ordering. When a discrete quantum of energy permittivity (a super string), is to bear a holomorphic propagation, in a certain number of anharmonic dimensional parameters, when going into BRST, then, the Betti Number, will, at that point in physical translation, be equal to the positive Imaginary Number, that is here to be tantamount, to that earlier implied certain number of anharmonic dimensional parameters. I will continue more with the suspense, Later! See you soon, in the upcoming paragraphs, illustrating ideas, appertaining to, as the discrete energy differentiates!!! Sam Roach! (1989).

Two different and distinct covariant Hamiltonian Topological Manifolds, are to be spontaneously undergoing respectively distinct and different dimensional compactifications, except that one of such individually taken actions of compactification, is to occur relativistically quicker, than the other of such respective individually taken actions of compactification. That Hamiltonian Topological Manifold, of which is here to be incurring its eminently corroborative act of decreasing in net spatial dimensionality, in a relativistically quicker rate, relative to the motion and presence of electromagnetic energy, will often tend to work to bear a stronger jump into the future, than the other of such comparative individually taken Hamiltonian Topological Manifolds, over its net Progression. 

Other Cool Ideas 2

 The Riemann-Based Remainder, of the harmonic component of dispersed homotopic residue, may be reductional in consideration, as being equivocal to charge residue, as taken in Coulombs. 

A super string basically amounts to being, 6.62604007149*10^(-34)(Joules Inverse Frequency). This is here to be considered, as being “The Planck Phenomenon.” Furthermore; Discrete Radial Energy, is (6.62604007149*10^(-34)(Joules Inverse Frequency))/2PI.

The general holomorphic direction, is in the relative I direction, or, in other words, the general holomorphic direction, tends to be, in the direction, that most facilitates, an eminently corroborative bearing, of optimum frequency. 

The general anti holomorphic direction, is in the relative -I direction, or, in other words, the general anti holomorphic direction tends to be, in the direction, that most facilitates, an eminently corroborative bearing, of optimum time. 

Frequency dispersion, due to the acceleration of a mass-bearing Hamiltonian Topological Manifold, tends to facilitate the incursion of the i*PI(Del)Action.

The phenomenon of a vibrating eigenstate, that is propagated through a delineation-based span, via its eminently associated frequency, may be thought of as being an eigenstate of motion inverse frequency, that is here to sequentially progress through a proscribed direction, over a corroborative set of iterations, as taken over a duration, that may be perceived of, as appertaining to the inverse eigenstate of its piecewise continuous periodical flow, to where the mappable region, that is here to be trekked by the vibrational flow, of the kinematically propagated eigenstate, of motion inverse frequency, over the span of relativistic time, is here to be equivocal to progressive inverse thought. 

The more meticulously piecewise continuous, that the vibrational propagation is to be expressed of as, over the general mappable course, of the eminently associated delineation-based span, that is here to be respectively trekked, when this is here to be taken, for an eminently corroborative, kinematically progressive, distributional set of cohesive discrete energy eigenstates, that the foretell of such a general case scenario, will often tend to spontaneously result, in a consequential enhancement of the  differential frequency, that is thereunto to be demonstrably expressed, by the Lagrangian-Based flow, of the propagational generation, that is here to be eminently related, to the kinetic transference of a cohesive set of discrete energy eigenstates, through the general medium of space time fabric, over the general venue of relativistic time. 

Degenerative frequencies tend to be more likely to exhibit greater entropy, than generative frequencies do. 

When frequency dispersion, due to the acceleration of a mass-bearing Hamiltonian Topological Manifold, is to be spatially convergent, this will often tend to be eminently corroborative, to the general incursion, of the generation of a hermitian i*PI(Del)Action. Furthermore; when such a respectively considered frequency dispersion, instead, is to be spatially divergent, this will often tend to incur the generation, of a spurious i*PI(Del)Action. 

Perturbative Inversion Of An Initially Real Riemann-Related Ricci Curvature

 The perturbative inversion of a given arbitrary state, of the initial tense of a Real Riemann-Related Ricci Curvature, may often, at times, be eminently associated, with the conversion of a set of one or more gravitational waves, into a set of one or more thought waves. SINCERELY, SAMUEL ROACH.(1989).

Spatial Dimensionality Of Neutrinos

In league with my particular model of string theory; Neutrinos tend to work to bear both a Riemann metric component, And, a Nijenhuis metric component. Although the Riemann metric component of a neutrino, tends to work to bear a lack of spatial dimensionality; The Nijenhuis metric component of a neutrino, tends to work to bear 12 spatial dimensions. This is facilitated, in part, on account of a phenomenology, that I call, the proximal local presence, of, "The Double-Helicit Calabi-Yau Manifold." For Instance; Do you recall how, at a reverse-fractal tense, DNA exists, as a double-helicit holonomy of topological manifold? Now; Take this down to the superstring-related level. Imagine a tense of a double-helix, yet, in this particular case, think of this in terms of the windings of superstring-related phenomenology. Even though such a supposed holonomic structure, were here, in a way, to have the workings, of a 12 spatial dimensional framework, the expressed nature of such a "double-helix" of a Calabi-Yau space, would work to form a tense of a Mobius-Related inter-relationship, as taken at the Poincare level, to the internal reference-frame of the relative Riemann vantage-point, when in relation, to the Poincare level of the internal reference-frame of the relative Nijenhuis vantage-point. Such an inferred tense, of a "Mobius-Related inter-relationship," would therefore have the tendency, of making the holonomic presence of the metric-gauge-related source, that is here to be of the angular momentum of such a neutrino, appear, via detection, to be "dimensionless," in spite of the physical condition, that at the perspective, that is Poincare to the internal reference-frame of the Nijehuis exhibition of such a neutrino, in a way, is here, instead, to be of a 12 spatial dimensional holonomic framework.THANK YOU! TO BE CONTINUED!SINCERELY, SAMUEL DAVID ROACH. 

Kahler Manifolds -- Aerodynamic

 Kinematically delineated Calabi-Yau Manifolds that are Kahler, have the general tendency of being more aerodynamic, than otherwise analogous Calabi-Yau Manifolds that are not Kahler. This is because such Kahler Manifolds, since these have a smooth Riemann surface, will tend to work to bear both less Chern-Simons Lagrangian-Based spurs and less Chern-Simons metric-based spurs. This just stated condition, works to facilitate the general physical condition, in which such mentioned Calabi-Yau Manifolds, will thereby consequently tend to work to bear both a more hermitian Lagrangian-Based spatial transfer, as well as tending to work to bear a more hermitian metric-based spatial transfer. This general condition, will consequently lead to the general physical attribute, in which such an implied Kahler Manifold, will thereby resultantly tend to spontaneously work to bear both a more hermitian angular momentum, as well as spontaneously working to bear a more hermitian spin-orbital momentum. This thereby tends to free-up the motion of such an inferred Kahler-Based Calabi-Yau Manifold, to where, as implied before,  it is thereby to consequently tend to end-up spontaneously becoming more "aerodynamic," than an otherwise analogous kinematically delineated Calabi-Yau Manifold. TO BE CONTINUED! SAM ROACH. 

Mild Hint

 What if it were possible, to harmonically synchronize the resonant pulsation of the given arbitrary emission source, of the respectively considered generation, of a directly associated Tesla surge(?); Could this general type of a Riemann-Based operation, potentially work, at least in part, to resultantly bear a spontaneously type of a harmonic alteration, in the initially considered surge of Tesla-Related Energy, to where this inferred harmonization of the initial flux of anharmonic electrodynamic energy, could thereby work to bear, at least to a certain amount, some sort of a decrease, in the initially inferred propagation of entropic electromotive flow? I realize that Newton's second law of thermodynamics indicates, that the net entropy that is exists in the universe can not be decreased, yet, is that really always actually the case? SAMUEL DAVID ROACH. 

Riemann/Rayleigh Scattering Of Cohomology-Related Flow

 Charge often tends to facilitate, the Riemann Scattering of a cohomology-related flow. Whereas; Entropy often tends to facilitate, the Rayleigh Scattering of a cohomology-related flow. SAMUEL ROACH. 

Recursively Re-Calibrated Chern-Simons Invariants, In Conjunction With Homotopic Residue

 The multiplicity of recursively re-calibrated Chern-Simons Invariants, when in conjunction with dispersed homotopic residue, of which is here to be scattered in a Riemann-Related manner, tends to work to facilitate the formation, of the general phenomenology of charge. Whereas; The multiplicity of recursively re-calibrated Chern-Simons Invariants, when in conjunction with dispersed homotopic residue, of which is here to be scattered in a Rayleigh-Related manner, tends to work to facilitate the formation, of the general phenomenology of entropy. TO BE CONTINUED! SINCERELY, SAMUEL ROACH. (1989).

Homotopic Dispersion -- Riemann/Rayleigh Scattering

 When a given arbitrary tense of homotopic dispersion is to happen, via a Riemann Scattering, this will often have the general tendency, of working to form magnetism, of which will tend to reverse-fractal into electrodynamic charge.  Whereas; When a given arbitrary tense of homotopic dispersion is to happen, via a Rayleigh Scattering, this will often have the general tendency, of working to form a local tense of holonomic disorder, of which will tend to reverse-fractal into entropy. TO BE CONTINUED! SAMUEL.

Perturbation Of Chern-Simons Invariants — Facilitated Scattering

 Harmonically perturbative Chern-Simons Invariants, may often have the general capability, of tending to work to facilitate, a tense of Riemann Scattering(s). Whereas; Anharmonic-Related perturbative Chern-Simons Invariants, may often have the general capability, of tending to work o facilitate, a tense of Rayleigh Scattering(s). I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL.

Stipulating A Yukawa Coupling -- Working To Involve The Product Of Relativistic Nijehuis Heterotic Strings

 Let us initially stipulate the potential existence, of both E(3)XE(3) heterotic superstrings, as well as the potential existence, of E(5)XE(5) heterotic superstrings. Let us next say, that one were to have a given arbitrary E(3)XE(3) heterotic superstring, as taken from one universal setting, to be heuristically coupled, via the general tense of a dual binary escalation, as this is when in conjunction with a given arbitrary E(5)XE(5) heterotic superstring, as taken from another universal setting (as taken from a different universal setting, than the other said heterotic superstring was here to be taken from). Let us now suppose, that a respective "observer," were to be somehow perceiving/detecting the given arbitrary respective coupling interaction, as again, via the said respective tense, of a dual binary escalation, as taken between these two different and distinct singular examples, of both individually taken inferred genre of heterotic superstring, -- to where the said "observer," is here, in this particular given arbitrary type of an example, to be both viably and intrinsically existent, as eminently to be considered, from within the general Ward-Cauchy-Related bounds, of the respective universal setting, that is here to be innately directly associated, with the Ward-Cauchy-Related physical bounds, of the same universal setting as the earlier mentioned E(5)XE(5) example, of such a heterotic string, that is here, in this particular given arbitrary case scenario, to be coupled, via the inferred escalation, in conjunction with the earlier mentioned E(3)XE(3) heterotic string. Let us now stipulate, that the just inferred Nijenhuis nature of the said E(3)XE(3) heterotic string, is here to be of an eminently heuristic relativistic complex nature, when this is here to be taken in relation, to the respective Real Riemann(Ian) nature, of the said E(5)XE(5) (heterotic) string, of such a given arbitrary case scenario. It consequently follows, that if these two just described individually taken superstrings, that are here to be of the just stipulated general nature, are to couple as such in a heuristic manner, the resultant Yukawa Coupling, that is here to often tend to come into play, will often, at times, have the general tendency, of working to form the equivalent effect, of the same type of a general Ward-Cauchy-Related behavior, as a heuristic E(8)XE(8) heterotic superstring will often have the capability of working to express. P.S. -- As A General Potentially Oversimplified Hint: -- [(e^(3i))^2]*[(e^(5))^2] = [(e^(-9))]*[(e^(25))] = [e^16] = [e^8]*[e^8]. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL ROACH.

Consonant Gravitational Vibrations Incurred Upon Mass-Bearing Energy, Via A Riemann Scattering

 When a given arbitrary general tense of a cohesive set of consonant gravitational vibrations, are here to be incurred, upon a Noether-Based mass-bearing cohesive set of discrete energy quanta, to where these are to interact with such an inferred "team" of discrete mass-bearing energy quanta, in such a general manner, in so as to work to form a relatively direct interaction, which may here to described of, as being, a certain particular genus of a Riemann Scattering, to where this reductional tense of a Wess-Zumino-Related action, may at times, often tend to form, what may simply be described of here, as being the resultant tangential propagation, of a set of one or more vowel sound phenomenology, of which may here, in this given arbitrary particular case scenario, be of the general nature, of having a basically inaudible respective proximal local eminent presence here. I WILL CONTINUE WITH THE SUSPENSE LATER(SOON)! (1989!).TO BE CONTINUED! SINCERELY, SAMUEL.

Heuristic Dispersion/ Inverse Dispersion

 An initial "bundle," of a topological grouping of entropic eigenstates, will often have the general tendency, of working to bear an ensuing spontaneous heuristic dispersion, over the respective duration, of a relatively transient Fourier-Related field progression. Whereas; An initial "bundle," of a topological grouping of relatively highly magnetic eigenstates, will often have the general tendency, of working to bear an ensuing spontaneous inverse dispersion, over the respective duration, of a relatively transient Fourier-Related field progression . A Heuristic dispersion, often tends to be associated with a Rayleigh scattering of physical eigenstates, as opposed to bearing an eminent association with a Riemann scattering of physical eigenstates. Whereas; An inverse dispersion, often tends to be associated with a Riemann scattering of physical eigenstates, as opposed to bearing an eminent association with a Rayleigh scattering of physical eigenstates. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SAMUEL DAVID ROACH.

The Riemann Cohomolgical Coupling

 When the kinematic action that is here to be undertaken, by the respective given arbitrary interdependent covariant motion, of two or more different and distinct cohomological eignenstates, that are here to be of the same universal setting, which is thereby to be physically translated, as this earlier mentioned kinematic action, is here to be directed towards each of such stated cohomological eigenstates, towards each other, to thence work to enhance the resultant interactive output, which is of the respective generation of their net tense of cohomological eigenstate, to where it is here to consequently follow, that one may then say that this general type of a Coupling, that is here to work to consequently tend to increase the net potential efficiency, that is here to be of the directly associated respective cohomological generation, to be of a genus of Coupling-Related Operation, that I will name here in my particular model of string theory, as being of the nature of acting as a Riemann Cohomological Coupling. (RCC). TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

As To Chi And Tense Of Scattering

 "Yin(g)" (which basically amounts to constructive "chi") tends to the general inclination of Wess-Zumino Interactions, -- which tends to the general inclination of Riemann Scatterings (harmonic scatterings), -- which tends to the general inclination of the multiplicity of creative forces (Forces that build things up). Whereas; "yang" (which basically amounts to destructive "chi") tends to the general inclination of Cevita Interactions, -- which tends to the general inclination of Rayleigh Scatterings (anharmonic scatterings), -- which tends to the general inclination of the multiplicity of destructive forces (Forces that break things down). I will continue with the suspense later! To Be Continued!  Sincerely, SAMUEL DAVID ROACH.

Homeomorphic Nature And Scattering

 When the Motion of a cohesive set of discrete energy quanta, is to be brought Into a tense of working to display a homeomorphic nature, this often tends to be the case, of a general genus of a  Riemann scattering. Furthermore; when the Motion of a cohesive set of discrete energy quanta, is to be brought Out of a tense of working to display a homeomorphic nature, this often tends to be the case, of a  general genus of a Rayleigh scattering. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

Diffeomorphism And Scattering

 When a cohesive set of discrete energy quanta, is to be brought Into a condition of diffeomorphism, this often tends to be the case, of a general genus of a Riemann scattering. Furthermore; when a cohesive set of discrete energy quanta, is to be brought Out of a condition of diffeomorphism, this often tends to be the case, of a general genus of a Rayleigh scattering. To Be Continued! Sincerely, SAMUEL DAVD ROACH. (1989). 

Harmonics Of Pressurized Vacuum Perturbation

 The general harmonic perturbation, of a given arbitrary tense of a Ward-Cauchy-related pressurized vacuum, tends to “move” in the “direction,”of inclining those effected discrete quanta of energy, that are thence to be directly influenced, by such a general genus of a given arbitrary tense of a harmonic perturbation, — to have an increased probability of tending to work to form the physical conditions, of working to bear a Riemann Scattering; Whereas — the general anharmonic perturbation, of a given arbitrary tense of a Ward-Cauchy-related pressurized vacuum, tends to “move” in the “direction,” of inclining those effected discrete quanta of energy, that are thence to be directly influenced, by such a general genus of a given arbitrary tense of an anharmonic perturbation, — to have an increased probability of tending to work to form the physical conditions, of working to bear a Rayleigh Scattering. SAMUEL.

Co-Tangential And Tangential Flow

Let us initially consider here, in this case scenario, that a given arbitrary physical phenomenon, of a given arbitrary tense of a holonomic substrate, -- is to be spatially translated into the relative forward-holomorphic direction.  IF such a set phenomenology is to be in the process of a tense of physical "scattering," then it follows, that; A Co-Tangential Flow tends to be more associated with a Riemann Scattering; Whereas, a Tangential Flow tends to be more associated with a Rayleigh Scattering. SAM.

Clifford Expansion, Relating To Rayleigh Scattering Of Component Parts Of Complex Manifolds

Let us initially consider a mass-bearing orbifold eigenset, -- that is here to act as the holonomic substrate of a complex manifold.  When those discrete quanta of energy, that are here to have worked to comprise such a said orbifold eigenset -- are to result in an action, by which these said quanta are to consequently diverge from each other, via a Rayleigh scattering, such an inferred general genus of a divergence, will often tend to be as appertaining to that of a general genus of a Clifford Expansion.  Furthermore; let us next consider a mass-bearing orbifold eigenset,  -- that is here to act as being of the holonomic substrate of a Real Riemannian nature.  When those discrete quanta of energy, that are here to have worked to comprise such a said orbifold eigenset, are to result in an action, by which these said quanta are to consequently diverge from each other, via a Rayleigh scattering, such an inferred general genus of a divergence, will often tend to be as appertaining to that of a general genus  of a euclidean expansion. To Be Continued! Sincerely, Samuel David Roach.