Showing posts with label ground-states. Show all posts
Showing posts with label ground-states. Show all posts

Friday, December 22, 2017

More As to The Idea Behind Substringular Recycling

Mini-Stringular segmentation is a general genus of phenomenology -- that is constantly being fed both into and out of both superstrings, first-ordered point particles, norm-state-projections, along with such a general genus of phenomenology as well as also being fed into other Ward-Cauchy-related phenomenology.   Such a constant re-distribution of mini-stringular segmentation, is part of what works to recycle substringular ground-states to norm-states -- and vice-versa.  Mini-Stringular segmentation is both: what works to form the holonomic substrate of substringular fields, what works to form the "yarning" of first-ordered point particles, what works to form zero-point-energy, etc... .  As far as I can currently surmise, the smallest phenomenology that can be divied-out, is on the order of mini-stringular segmentation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Friday, October 17, 2014

Part Three of the Interim Between Course 17 and Course 18

The condition of the recycling of ground-states converting into norm-states and vice-versa works to cause a flow of the directly corresponding indices -- these indices of which move in such a manner in so as to reach a relative center-state, which localizes toward the activity of that permittivity which exists as to where the correlative ground-states are most prime.  Meanwhile, the correlative norm-state-based associations work to cause Real-based first-ordered point particles to be over half of being fully compactified -- while at the same general genus of metric, working to make the correlative Fock-based states to be less than half of being fully compactified.  This is because the directly associated covariant differential geometries that work to correlate the so-stated ground-states with the so-stated norm-states works to allow for a more "ionic" distribuation of condensed oscillation, -- even though any viable wave distribution must bear a certain level of quantum-based state of conservation, over the course of space and time.  This works to make a condition of indistinguishable replacement, as to the conformally invariant manner of the maintanence of those ground-based states that work to comprise any give arbitrary superstring of discrete energy permittivity.  This process of the recycling of ground and norm states -- the one general genus of state to the other and vice-versa, pertpetually -- works to involve from one relatively Real-based state to many Fock-based states, to vice versa, over the eigenbase of certain of those gauge-metrics that are most activated over the generally reiterative metrical-based activities that happen during the generally unnoticed durations of Ultimon Flow.  This acts as if a given arbitrary respective set of substringular globalizations were to be exerted upon the directly corresponding net field impulse range -- and thus, part of the reason as to why I call a layer of reality that is to exist from within a set of parallel universes as being termed of as a tori-sector-range.  I will continue with the suspense later!  To be Continued!  Sincerely, Sam.

Wednesday, June 27, 2012

Part Two Of The Seventeenth Session Of Course Ten

As I was discussing, as the discrete units of the directorals that here correspond to the prior eluded tensors are considered over an arbitrarily given Fourier condition that inter-relates the related superstrings that work to comprise the assoicated said traits, residue that is here delineated over a relatively brief metric works to transversally and vibrationally commute a certain degree of "tingling" that lubricates the kinematic association that covariantly binds the two said traits.  The coupling that happens over the course of the prior mentioned brief metric is an arbitrary given example of a Yakawa coupling that here involves indices that works to allow a variance that translates a tense of Weyl covariance that tends to conform to the corresponding Ward Caucy conditions that work to define the physical boundaries of the said traits in all of the Fourier-based derivatives that involve the overall dimensional scope in which the superstrings that work to define the said traits exist in.  The corresponding Cassimer Invariance that will happen here -- if the related Yang-Mills supersymmetry is to here take hold -- will then attain a spontaneous metric that here involves a parity and dual chirality that will work to even out the loci of the settings over the duration in which each associated encodement is quantized.  Yet, if the corresponding Yang-Mills supersymmetry that we are to consider were to not be attained here, then the associated holomorphic residue will flow over the duration of the brief metric that inter-relates this second possible scenario -- after each reiteration that would thence happen between the homotopic indices of the said traits.  The prior mentioned metrical condition would cause the metaphorical-based "fluid" flow that I had initially mentioned in my last post to become perturbated in terms of its displacement over a tightly-knit Fourier Transformation in which the traits mentioned earlier will, in this case, not be as superconformally invariant as these otherwise would be.  Under the conditions of such a perturbation of what would otherwise be more delineatorial-based stable, the inter-related fractal of magnetic coupling that could be extrapolated here would involve an increase in magnitude as well as an increase in terms of the corresponding fractal of charge.  The "fluid" would then snap and recoil in terms of its delineation over the course of the prior mentioned tightly-knit Fourier Transform.  If the associated holomorphic index that would then exist under the directly prior mentioned conditions were to now increase in terms of action intensity over the course of the kinematics that would involve the covariance of the related eigenstates that are comprised in part by the superstrings that work to form the prior mentioned said traits, then the recoiled sections of "amorphous" quantitative topology may -- after the coure of the proper sequence of iterations and the proper series of wave discharge -- slip in terms of its positioning of local distribution as a folded manifold to where it would go back into a connection that would here exist in-between the hyperstates of the said traits in so that the exterior counterpoise that would here be physically present, as well as the corresponding hypnostates of the related holonomic ground-states, would then differentiate through time in a singularized manner in so that the given phenomena would then act as a theoretical homotopical-based eigenbasis.  Such an eigenbasis would here be partially codifferentiable in terms of the inter-relation of the covariance of the two said traits over a related Fourier Transformation in such a manner so that the related activity would work to draw in the quanta of a re-convergent norm projection. I feel that I am burning the candle at both ends.  I will continue into course 11 when my sanity lets me.  I will continue with the suspence later!  Sincerely, Sam Roach.

Thursday, February 3, 2011

Part Four of the Fourteenth Session of Course Six

Well hello again world, this is Samuel David Roach here!  Happy to be back!  Here we go!

               
Superstring-related ground-states that are indistinguishably different through a successive series of iterations, when not considering alterations in metric-gauge quanta and exterialized filled permutations by the related Fourier Transformations that happen to the given ground-states in the delineatory translation of the given ground-states in the course of their redistribution through the multiplicit operand of space, are superstrings that are detectable as relating to light matter and light energy.  (These are the illuminated superstrings.)  Superstring-related ground-states that are distinguishably different, through a successive series of iterations, in terms of the permutations that are Gliossi to the holonomic structure of the described superstrings over the related Fourier Transformations, that happen to the ground-states in the delineatory translation of the given ground-states in the course of their redistribution through the multiplicit operands of space, are superstrings that are detectable as relating to dark matter and dark energy.  Exterialized field permutations here are alterations in the fields that surround superstrings, yet are not appertaining to the topological Laplacian mapping of the here mentioned superstrings themselves, while permutations that are Gliossi to the holonomic structure of the described superstrings are alterations in the topological Laplacian mapping of the here mentioned superstrings themselves -- whether the exterialized fields appertaining to the associated superstrings here may or may not be altered in terms of the mini-string interactions in a Fourier tense, or altered in terms of the mini-string relativistic delineations as taken in a Laplacian tense.  Because I love the Human Race!
Sincerely, Sam Roach.                                                                                                          

Monday, January 31, 2011

Part Three of the Fourteenth Session of Course 6

Well hello again world, this is Samuel Roach here!  Glad to converse with you!  Here comes part three!
            
Superstrings release the residue of their ground-states during the sub-metric that transpires during the Bases of Light because illuminated superstrings are almost always in a Main World Tube & because illuminated superstrings always acquire the residue of their respective tori-sector-ranges that is essential for the recyclling of differential geometries, and differential geometries recycle to allow for the Bases of Light.  You see, since the most overtly recycled ground-states are, as a fraction of the sum of all matter and energy, equal in quantum to the fraction of the back-and-forth sways that are released from the Klein Bottle during an eigenmetric of the Kaeler-Metric versus those associated back-and-forth sways that are fully confined in the Klein Bottle during the mentioned eigenmetrics of the Kaeler-Metric.  There are constantly Gaussian Transformation occurring.  This is a 15 to 1 ratio -- fifteen times as much dark matter and dark energy as light matter and light energy.  The integration of light's basis is light.  Light is the basis of perception.  Perception is the basis of communication.  Communication (here, specifically commutation) is the basis of iteration and reiteration.  Reiteration is the basis of prolonged existence.  Prolonged existence is the only way a reality can begin and continue.  The reason for the reverse-fractor relation of the Kaeler-Metric to the ration of dark matter and dark energy versus light matter and light energy is that the basis of Ward Polarization is equal to the fraction of relatively mildly worked upon recycled ground-states to relatively overtly worked upon recycled ground-states.  Also, there is fifteen times as many Hodge Indices related to norm-states as the Hodge Indices related to ground-states when one includes the Fourier Translation of states in both the Main-World-Tubes as well as in the Royal Arc.  I provide a more rigorous explanation as to why this is the way this is during the publishing of the fourth part of this session.  I will continue later with the fourth and last part of this session.  Until then, you have a phenomenal day!  God bless you in the name of Yahweh!  Sincerely, Sam.                                                                          

Wednesday, January 12, 2011

Part One of the Test Solutions For the Second Test of Course Six

1)  The number of stringular mers that comprise a particular substringular encoder determines the number of instantons that it takes for a particular ground-state to recycle into its opposite type of state of tangency and back.
If a ground or a norm-state switches in tori-sector-range that these correspond with, the total number of instantons required for full recycling will equal the total number of substringular mers existant in the framework of the multiple substringular encoders that such a perturbated superstring directly associates with over a set sequence of unitary Fourier differentiation that locally maps out the recycling of one ground-state or locally map out the recycling of one norm-state.

2)  Ground-States and Norm-States.

3)  Norm-States recycle into ground-states involved with the kinematic sequential series of the local group Chi-Shaped-Trace, while then recycling back into norm-states via their local group cross-section that is directly involved with the Royal Arc.  Each step of such recycling happens during the sub-metric that happens during the duration that happens via the sub-metric that is directly associated with the Bases of Light, -- and in an indistinguishably different manner so that order is maintained in the localization of covariant norm-states and ground-states.

4)  Ground-States are recycled as in "3," except that these initially recycle into norm-states via the Royal Arc, while then recycling back into ground-states via the local group Chi-Shaped-Trace associated with the corresponding Basis of Light that the described ground-states are associated with (ground-states that return to their home-tori-sector-range are recycled into norm-states and then back into ground-states that are directly associated with their original Home-Basis of Light), during its metrics -- such a trace existing in the general locus of the Main-Heterotic-String-Fabric.

The next four test solutions will be provided in the next post, while the last four test solutions will be provided in the post after that.  I will continue with the suspense later!  Until then, you have a phenomenal day!
Sincerely, Sam Roach.                                                                               

Sunday, January 9, 2011

Test Questions For The Second Test Of Course Six (6)

1)  What factor allows one to know how many instantons of a set tori-sector-range needs to iterate  in order to define when a first-ordered point particle of a superstring, of the described tori-sector-range, will be recycled  from being converted with indistinguishable difference into a different form of differential geometry while then being recycled back with a similar tense of indistinguishable difference back into the same general format of differential geometry?

2)  What are the two general differential geometry types?

3)  Describe in general how norm-state-related first-ordered point particles of the substringular are recycled.

4)  Describe in general how ground-state-related first-ordered point particles of the substringular are recycled.

5)  When both limits of the Royal Arc are commuted through recycling, what is this shape?

 6)  What is this prior mentioned shape in reference to test statement "6" as integrated along one general main world-sheet?

7)  Describe why there are, in-between the durations of each instanton, instanton-quaternionic-field-impulses.

8)  Describe how tori-sector-ranges vary in flow.

9)  Describe why a "steady-state" related superstring must constantly, in-between the duration of each instanton,  travel along the whole orbit of the Continuum.

10)  What fascillitates the binding of superstrings in the globally distinguishable?

11)  Why must substringular travel be almost instantaneous in terms of our terrestrial time?

12)  Why is dark phenomena essential in order for any phenomena to exist at all under our present conditions of time and space?                                                                                                            

Monday, December 27, 2010

Part Two Of Session Nine Of Course 6 (6)

Well hello again world, this is Sam Roach here to provide for you the second part of the ninth session of Course Nine!  I hope that my method of conveying information and knowledge makes it relatively easy for at least some people to see the gist as to what I am trying to teach!
            
As an example of the recycling of a ground-state gauge-condition converting into a norm-state gauge-condition, which will also give you the gist as to how norm-state gauge conditions recycle into ground-state gauge-conditions, I will provide an example that will help the reader to grasp a little bit better what I just recently tried to convey.:  For instance, if a norm-state were to be illuminated at one instant when there were 10^(43) general eigenstrings in a corresponding substringular encoder that is related to one tori-sector-range, then it would take one second for the described norm-state's holonomic topological fabric itself to recycle from the condition of being a norm-state to being a ground-state back to being a norm-state.  Yet, extrapolation methods would not be able to directly detect such changes in the associated norm-state field on account of indistinguishable differences.  Or, for instance, if a norm-state were to be illuminated at one instant when there were 10^(40) general eigenstrings in a corresponding substringular encoder that is related to one tori-sector-range, then it would take one millisecond for the described norm-state's holonomic topological fabric itself to recycle from the condition of being a norm-state to being a ground state back to being a norm-state.  Respectively, if a ground-state were to be illuminated at one instant when under the two prior individually taken conditions, the first proscribed ground-state would recycle its holonomic topological fabric itself from ground to norm to ground in one second, while the second proscribed ground-state would recycle its holonomic topological fabric itself from ground to norm to ground in on millisecond.  When a norm-state or a ground-state redelineates from one tori-sector-range to another, it will take two whole seconds for its holonomic topological substance itself to recycle fully if both of the related substringular encoders contained 10^43 eigenstrings in a corresponding substringular encoder, two milliseconds for its holonomic topological substance itself to fully recycle if both of the related substringular encoders contained 10^40 eigenstrings, and 1.001 seconds for its holonomic topological subsance itself to fully recycle if one of the related substringular encoders contained 10^40 eigenstrings while the other related encoder contained 10^43 eigenstrings.  This holds true only under the conditions of one discrete unit of time being exactly 10^(-43) seconds.  As described before, we only generally notice activity that happens from within the Main-World-Tubes.  The Royal Arc, the Main Heterotic String Fabric, and the hoops that contain the substringular encoders are -- for all practical purposes -- undetectable by us under normal conditions.  What I mean by a full recycling of the holonomic topological substance of a norm-state means that the mini-string or substringular field of such a superstring taken as specific covariant entities that are mapped out in terms of their redistribution and redelineation -- although indistinguishably replaced to allow for a minimization of excess entropy -- takes anywhere from one millisecond to two seconds for the whole process of being converted from its here original norm-state-based phenomenon to a ground-state-based phenomenon then back into a norm-state-based pheonemenon.  This is only under the conditions that only two layers of reality are shared by the indistinguishable replacement of mini-string for a ground or a norm state over the course of about two terrestrial seconds -- if you get my drift. Yet this does not necessarily mean that the recycled norm-state here described is relocalized back into the identicle Fourier Translation of where its original covariant-based field was located.  The same is true for the full recycling of ground-states, except that the mini-string of ground-states recycles into norm-states that reconvert back into ground-states.

The reason as to why there must be a Royal Arc is that the number of second-ordered point particles that exist in the Main Heterotic String Fabric -- which is where superstrings are pulled into association with all three sets of parallel universes in-between the course of each instanton, and is also the general region where norm-states convert most directly into ground-states, while also acting as the basis of the jointal translation of phenomena -- must be counterbalanced by the same number of second-ordered point particles that exist within a relatively smooth-curved Ward Neumman Bounds that acts to most directly recycle ground-states into norm-states.  Once norm and ground states convert into ground and norm states, these states -- in terms of their holonomic topological substance -- convert back into norm and ground states that are correspondingly localized, under the conditions of indistinguishable covariant codifferentiating differences, at whichever locus such eigenstates of gauge-action are encoded to be at according to the combined conditions of the Laplacian and Fourier Translation of the substringular encoders, the Laplacian and Fourier Translation of the said holonomic topological phenomena in terms of the substringular association that exists in the integrable summed partial differentiation of superstrings with their corresponding "mini-bases" during the Bases of Light, the multiplicitly applied covariance of imaginary supercharge in terms of all of the effective Real Reimmanian  and Njenhuis directoralizations that such eigenstates of charge bear permittivity within and/or amongst each other, and, the Laplacian and the Fourier Translations that are associated with the status of orientation of the given superstring -- orientable superstrings obey Noether Flow, while unorientable superstrings are tachyonic.  I would think that I've described enough today!  Study hard -- Test Two of this course will be two sessions from now!  God Bless You, and you have a phenomenal day and a merry new year!  Sincerely, Sam.