Showing posts with label worm-hole. Show all posts
Showing posts with label worm-hole. Show all posts

Saturday, October 22, 2022

Facilitation Of Creating A Worm-Hole

 A balance between the right interdependent inter-relation, that is to exist, amongst a quickly paced rotational-based recursively smooth Ricci Flow, when in conjunction, with a quickly paced transversal-based recursively smooth Ricci Flow, may, at times, be capable of tending to help facilitate, the creation of a worm-hole. TO BE CONTINUED! SINCERELY, SAMUEL ROACH. 

Saturday, December 26, 2020

“Wear-And-Tear” Upon A Worm-Hole

 The multiplicity of the general interaction, of entropic tachyon-related photons (which tend to bear the combination, of having both a Khovanov geometry, along with a  Kaluza-Klein light-cone-gauge topology), with discrete energy quanta, that are here of the nature of working to bear a tachyon-related tense of kinetic energy (which tend to bear the combination, of having both a Khovanov geometry, along with a Yang-Mills light-cone-gauge topology), — works to facilitate the general processes, by which the “wear-and-tear,” that is here to be attributable, to what may often tend to happen to a worm-hole, when it has been utilized enough times, is often thereby to be able to happen to such a space-time-related “shortcut,” if it has been exacerbated, over the potential combination of both a lot of usage, along With a long duration that it may have been present, at some given arbitrary covariant region of space. Sincerely, SAMUEL DAVID ROACH.

Friday, May 17, 2019

Reverse-Fractal Of A Light-Cone-Gauge Eigenstate

When a worm-hole is artificially gauged -- right before it is utilized -- it acts like a major reverse-fractal of a light-cone-gauge eigenstate!  To Be Continued!  Sincerely, Samuel David Roach.

Saturday, May 7, 2016

Worm-Holes Linking Various Layers Of Reality

Unless one is traveling into the future in the same universal setting, when one is to travel through a given arbitrary worm-hole -- in so as to either go from one universal setting to another Or in so as to go to another spot in the same universal setting -- as to what the layer of reality one is to be going into, in either the respective newly entered universal setting or into a different spot in the same universal setting, the layer of reality that one will then ensue to be going into will often tend to be of whatever the predominant layer of reality is for the traveler, for the universal setting that the traveler was existing in right before her or she was to enter the so-stated given arbitrary worm-hole.  I will continue with the suspense later!  To Be Continued!
Samuel David Roach.

Friday, May 6, 2016

Worm-Hole Projections, the Last Part Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

Depending upon the manner of the trajectory of any one given arbitrary worm-wole that is to be formed, its projection often may or may not work to inter bind two different universal settings -- via the Fourier-based activity of the manner of the respective contorsioning that is to happen here, with whatever the said worm-hole in question would happen to be.  If the contorsioning of the Njenhuis-based Lagrangian-affiliated tensors, that are of the Doubolt-affiliated tense of that bending of  space-time-fabric that is to be utilized -- in so as to work to inter bind two different relatively distant spots in the  Continuum -- is to here work to bear a Li-based tense of Chern-Simons singularities, then, the so-eluded-to worm-hole will then often tend to work to interconnect two different settings that are likewise and respectively of two different universal settings.  Yet, if the contorsioning of the Njenhuis-based Lagrangian-affiliated tensors, that are of the Doubolt-affiliated tense of that bending of space-time-fabric that is to be utilized -- in so as to work to inter bind two different relatively distant spots in the Continuum -- is to work to bear a Li-based tense of hermitian  singularities instead, then, the so-eluded-of worm-hole will then often tend to work to interconnect two different settings that are likewise and respectively of the same universal setting.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Wednesday, April 27, 2016

Part Thirteen Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

The earlier mentioned "Sterling Lagrangian" or "Sterling Hamiltonian Operand" related Ward-Caucy-bearing condition of a worm-hole, works to for a loop -- that bends without the added set of Ward-Caucy conditions that would here be working to form what would otherwise be a tense of jointal-based-space-time-fabric, -- since the contorsioning or the bending of space-time-fabric, that is directly associated with the Fourier-based differentiation of a worm-hole, is of a Doubolt-based nature, -- that will here tend to be piecewise continuous in a manner that does not tend to cause the Laplacian-based conditions for any spurious Lagrangian-based Chern Simons singularities, from within the Li-based setting of the general Hamiltonian-based field operation, that would work here in so as to operate in so as to help to form the torsional toroidal-based leveraging and pulley-based set of wave-tugs/wave-pulls(pushes), -- that would here work to form that general tense of gyration/oscillation-based Hamiltonian-based operators, that would here function in so as to bring the incoming holonomic substrate of phenomenology towards its furthered positional-based destinations of exit.  This would then tend to work to make the light-cone-gauge topology of any given arbitrary worm-hole, to be basically of a completely Yang-Mills or of a non abelian-based nature.

Tuesday, April 26, 2016

The Thrilling Part Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

In a certain sense, the toroidal-based compilation that works to form the holonomic substrate of the phenomenology of a worm-hole -- is an integration of what would otherwise act, as the integration of torqued semi-Laplacian-based orientifolds -- these of which would then work here to form the surrounding light-based energy, that works to encapsulate the semi-anuulus of the said given arbitrary respective worm-hole -- by which the entering phenomenology that is to be transferred through the so-stated worm-hole is to be pulled through, by the performance of a multiplicit "Green Function" that exists as a semi-Fourier differentiating "Sterling Lagrangian (or Sterling Hamiltonian Operand)," that works here to bear torsional toroidal-based flaps, -- that are here to be formed out of space-time-warped "Wilson Lines" that are here to be shut at the end of the worm-hole, where the entering phenomenology has come in --- to where the automation of the torsioned "Wilson Lines" that are of the so-stated worm-hole, are to then gyrate and oscillate in such a manner -- that works to act as a kinematic "screwing process," that works to both leverage and pulley the holonomic substrate of the entering phenomenology, in so as to re-translate the contorsioned or bent space to a furthered space-time-bearing of position, in so as to open at the point of re-entry, -- whereupon, the so-stated respective worm-hole as a whole is to at least temporarily be closed.  To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.

Tuesday, April 19, 2016

Part Eight Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

A worm-hole works to bear a set of orbifold eigensets, that differentiate in a Fourier-based manner in so  as to being a group-associated metrical-gauge-based Hamiltonian operator -- in so as to act, as well, as one overall Hamiltonian operand -- that behaves as one overall general genus of what may here be considered as the equivalece of a field-based transmitter, that also works to pull those phenomenology of a holonomic substrate that are to initially enter the depth of the semi-anuulus-based region of the said worm-hole, through a controrsioning or in other words throgh a bending of space-time-fabric, that works to translate the so-eluded-to Gaussian indices of the said entering holonomic substrate, in a kinematic manner, that pulls these said individually taken spaces through a mappable Lagrangian-based path, in a kinematic manner, into what would here tend to end-up being a completely different spatial region as to the destination-based volumed region where the so-stated holonomic substrate of entry is to end-up exiting the said worm-hole at.  This happens, in so as to make a projection of a Njenhuis tense of a Doubolt cohomological-based mappable tracing -- as to the physical mapping of the trace of one entity that is to then be transferred from one physical locality to another -- to happen, via what would mainly be due to the Fourier-based differentiation of a Minkowski-based bending of space, that is to here convey a directly corresponding Gaussian set of physical indices that are to here be translated from one spot to another -- in what would tend to be a difference of the equivalence of practically zero terrestrial-based time.  The spatial complexity of the Njenhuis tensorism of such a spatial contorsioning, would tend to involve two more sets of complex roots per eigenpulse of the self-same given arbitrary worm-hole, than the Real Reimmanian-based translation for a p-field would otherwise tend to bear, when this is taken under its directly corresponding Ward-Caucy-based conditions (this being that of the respective given worm-hole) -- which would here tend to make such a general state of a worm-hole to act as the equivalence of a heuristically majorized Hilbert Space.  To Be Continued!  I will continue with the suspense later!  Sincerely, Samuel David Roach.

Friday, September 4, 2015

Part Four of Session Seven of Course 19 -- The Klein Bottle and Orbifold Differentiaion

A supremumization is when one integrates a physical space into three extra spatial dimensions.  So, if one were to take a supremumization of a supremumization of an initial six spatial dimension-based Minkowski Space -- one will then have a twelve dimensional-based Minkowski Space.  Such a just eluded-to twelve-dimensional Minkowski surface or flat-based surface may often be considered as a volume-based space or a Hilbert Space,  instead.  (A Minkowski Space is a flat-based space, and, a Hilbert Space is a volume-based space.)  So, if one were to be initially considering a ten-dimensional Hilbert Space -- that is subsequently double-integrated into two additional spatial dimensions, into what will then be a twelve-dimensional Hilbert Space -- then, what this will here amount to, is the generally taken Laplacian-based condition of having the extrapolation of a majorization of a ten-dimensional volume-based space into a twelve-dimensional volume-based space.  One can have a flat space that may have up to 26 spatial dimensions, plus time.  The condition as to whether or not one is dealing with the consideration of either a flat-space or a Minkowski-based space or a volume-space or a Hilbert-based space, is whether or not one is either to be able to or to not be able to treat the space-time-based fabric in which one is to go through, over time, as a contortable sheet that is not viably travelled through in a transversel-based manner otherwise, or, instead, if one is to treat the space-time-based fabric in which one is to go through, as actually being a viably travelled through operand -- that would here be traveled through in a transversel-based manner, respectively.  A volume-based space or a Minkowski Space is most associated with a worm-hole that would -- in this case -- bear all of its additive source of velocity to the condition of the bending of space-time-fabric.  Yet, if any of the additive source of the velocity at all that is caused by the activity  of traveling through a given arbitrary worm-hole is due to a respective given arbitrary tense of a tachyonic propulsion, then, the manner of describing the nature of the space that would here be traveled through, would be a twelve-dimensional volume-based space or a twelve-dimensional Hilbert space -- when this is not including the dimensionality due to time itself.

Monday, November 12, 2012

A Little Addendum As To The Directly Previous

The tendancy of the general operation of Noether Flow is the baic manner that superstrings "like" to move in -- unless an outward source directly interacts in such a manner so that such a tendancy is not held due to phenomena being perturbated out of it.
The tendancy of Noether Flow does not include the initial activity that happens in the specific locus of photons in the first 384 instantons after these have struck another phenonenon, even though photons, when detectible, move slower when moving through a medium that is not either a vacuum or a contorsionable spatial entitiy.  Yet, outside of the two prior conditions, Noether Flow is the general tendancy as to the format of the operation of the motion of superstrings.
This is why point particles, when these are effected in a certain general manner by reverse-magnetism, not only tend to remain in the same universe that such a given arbitrary situation of superstrings started in under the initial conditions that I had mentioned, yet, such point commutators also tend to not be tachyonic unless these are perturbated upon by an outside source.
Point commutators, since these work to allow for the motion of superstrings through Ultimon Flow, tend to have the general flow of the superstrings that these are most directly affiliated with.
The directly previous statement is only considering a relativlely transient period in which the condensed oscillation of the mentioned given arbitrary point commutators is indistinguishably the substrate that works directly with their corresponding superstrings.
The condensed oscillation that comprises point particles of the first-order is constantly being recycled in a manner that is indistinguishaly different.
Such recycling works to allow a continual exchange of norm-states to ground-states and back.
Such a continual exchange works to allow for that Cassimer Invariance that works to allow electromagnetic energy to bear its relativity condtitions upon superstrings, in a manner that does not fray superstrings.
Special relativity works to effect the abelian conditions of superstrings so that the fractal modulae of superstrings is not overstrained.
This is why, although superstrings of mass may be translated faster than light, these mass-bearing strings may not actually go faster than light as a mass.
The condition of tachyonic propulsion is the condtition of a temporary alteration of the topology of the local light-cone-gauge for a certain limited quantum of mass-bearing superstrings that is brought back to its original abelian topology.
The temporary tachyonic motion of superstrings that are undergoing a Calabi interaction is not what I mean by a tense of tachyonic propulsion.
A mass as a mass bears a Kaluza-Klein topology.  (Abelian).
A mass is translated as a massless phenomenon going in a tachyonic manner only when bearing a Yang-Mills topology.(Non-Abelian).
A mass, when slowed under light speed, bears a Kaluza-Klein topology. (Abelian).
Light and kinetic energy bear a Yang-Mills topology.(Non-Abelian).
As an anzantz, a vast majority of the velocity of a worm-hole is the contorsioning of space, and not tachyonic propulsion, yet, tachyonic propulsion still exists.
Sincerley,
Samuel David Roach.