Part One Of Session Seven Of Course 20

Light, or any other form of electromagnetic energy, can scatter upon either phenomenology of mass, phenomenology of plain kinetic energy, or upon phenomenology of other electromagnetic energy -- over time.  When electromagnetic energy is to scatter upon another phenomenology, it is to strike the externalized core-field-density of the light-cone-gauge eigenstate of the discrete energy quantum -- that it is to come into contact with in the so-inferred Gliosis-based manner.  Furthermore, any electromagnetic or electro-dynamic energy will tend to scatter upon any discrete quantum of mass, kinetic energy, and/or electromagnetic energy, in an initially Rayleigh-based manner -- when it is to strike the just inferred multiplicit externalized field of such a light-cone-gauge eigenstate, over any metric that may be gauged of as an even Hamiltonian operation, around the instance of contact, in which the so-eluded-to set of one or more photons are to make a direct Yukawa-based coupling upon the said phenomenology that may here be either as a quantum of a mass, a quantum of kinetic energy, and/or a quantum of electromagnetic energy, over time.  This is particularly the case, when the phenomenology that is to be struck is in the Lagrangian-based path -- as to the mappable-tracing of the electromagnetic energy that is in its venue of moving in the direction of least time, as a Hamiltonian operand -- in which the photon or the photons that are to be scattered, are here to be "toggled" as is as according to Snell's Law.  Mass-Bearing superstrings of discrete energy permittivity, that are in a state of superconformal invariance -- tend to be Yau-Exact.  This is why I term those substringular manifolds, that are to be comprised of here as  mass-bearing strings -- as Calabi-Yau manifolds.  Electromagnetic superstrings of discrete energy permittivity, that are in a state of superconformal invariance -- tend to be partially Yau-Exact.  This is why I term those substringular manifolds, that are to be comprised of here as electromagnetic strings -- as Calabi-Calabi manifolds.  Furthermore, -- kinetic energy-bearing superstrings of discrete energy permittivity, that are in a state of superconformal invariance,  tend to veer into a condition of bearing Chern-Simons singularities.  This is why I call those substringular manifolds, that are to be comprised of plain kinetic energy -- as Calabi-Wilson-Gordan manifolds. 
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

First Two Test Solutions -- Test One Of Course 20

1)  The Fujikawa Coupling is a Ward-Caucy-based inter-relationhip, that is of the nature of that general genus of activity that is to happen in the substringular, when the two correlative ends of the open-loop phenomenological stratum of one discrete quantum of the kinetic energy permittivity of an electron -- that is in the process of being released from that said electron -- are to be brought together in a hermitian manner, via two covariant zero-state norm-state-projections, in such a manner in so as to help at working to form what is here to be the resulting holonomic substrate of one discrete photon.

2)  In any medium other than a vacuum, in which the light that is here to be traveling through such a medium, is here to be moving through the processes of Noether Flow over time, -- to where the said light is to go from initially scattering upon the holonomic substrate-based phenomenology of such a medium, while then going into a manner of then re-quantizing with other electromagnetic energy that is proximal local to the direction of the propagated motion of the said light, while then traveling in a relatively optimum-related "straight" manner until it is scattered again, and so-on, -- to where this is to happen in such a manner in so as to bend as little as feasible as is according to Snell's Law -- as it is to travel through "the direction of least time."

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Session 5 Of Course 20 -- Calabi Manifolds And Interactions

Light in a vacuum of space travels at 3.0*10^8 meters per second.  When light enters a medium that is not electromagnetic energy while it is also not a worm-hole, the light will tend to travel at a speed that is less than light speed.  For instance, when light strikes air, the light not only bends to a slight extent, it will also slow down to a correlative extent as well.  Once that light strikes the air, it will scatter -- while then subsequently tending to re-quantize to form light again.  Once the light reforms as light again, it will tend to travel in what amounts to as its given "tense of bend", yet in segmentations that are each of a relatively straight line, -- to where the said light, as it is here to be as is according to Snell's Law, is to then to go just slightly less than what light speed would be in a theoretical vacuum, as the so-eluded-to electromagnetic energy is to travel in the direction of "least time," as it is to only slow down and change direction, after each of such scatterings of the said light upon the so-eluded-to Calabi-Yau phenomenology of the said air molecules that it is to strike in a Gliosis-based manner over time.  For example, let's say that the given air was homogeneous in density, and that the light that I am referring to here did not have to significantly re-scatter again in the air, as the given light is here to be propagated downward toward the earth.  The light in this case is propagated towards the face of a body of water.  When the light strikes the water initially, the light will scatter, while then re-quantizing back into a beam of light that bends as is according to the density of the water -- and slows down as is according to this same density of the water.  The beam of light may be able to do this, if it is also not scattered by any plain kinetic energy, -- as other beams of light are to be inter-playing in this case scenario as well.  This beam of light may propagate until it is fully absorbed, most potentially by some alterior Calabi-Yau  space of mass.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Five Of Session 3 Of Course 20 -- Calabi Interactions

If the given medium that a beam of light is traveling through is not of a pure vacuum of space, -- in a way, then the said light will then work to depict an optical illusion of both when and where and what, that the specific circumstances were, that are to here be depicted by this respective given arbitrary beam of electromagnetic energy, that is to here work to illuminate the respective arena of what is to here be seen. This is again, because as light is traveling through any medium besides of a pure vacuum -- then, it is to tend to both bend and slow down, as is as according to Snell's Law.  Furthermore, the further away that the circumstances were by which the illuminated medium had worked to be penetrated by the said respective given arbitrary electromagnetic energy of such a case scenario, -- the longer ago that what was observed by the means of that illumination -- that was caused by the said beam of light, had actually happened, as may be in part extrapolated by the Lorentz-Four-Contraction that is to here be associated with the equation:
t = (1-(v^2)/(c^2))^.5
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Two Of Session 3 Of Course 20 -- Calabi Interactions

When light, or any given arbitrary electromagnetic energy, is beginning to travel through a medium of space -- that is not of a pure vacuum -- that respective phenomenology that the said electromagnetic energy is to here be traveling through, will tend to bend the so-stated electromagnetic energy to a certain extent.  This said tendency of light to bend, in any medium that it is to be traveling through besides a pure vacuum -- is as according to what is known of as Snell's Law.  In the process, -- the here relatively bent light will, as well, tend to be slowed down also, which is also related to what may be extrapolated by the math as to Snell's Law.  If light is to be bent by a homogeneous medium, in which Snell's Law is to here theoretically remain constant -- in so long as that light which is to here be traveling through the respective given arbitrary medium that is to here not be of a pure vacuum, is to continue to be moving through the so-eluded-to medium -- then, both the general tendency of the bending of such light, as well as the general tendency of the slowing of such light, will here tend to be remaining as relatively constant.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Five Of Session 1 Of Course 20 -- Calabi Manifolds and Calabi Interactions

As one one-dimensional superstring of discrete energy permittivity is being released from the Ward-Caucy bounds, of any respective one directly corresponding electron -- the local centralized knotting of the Rarita Structure eigenstate, that is most directly affiliated with the locally associated Fourier-based differentiation, that is of the said respective electron -- is relatively discombobulated from its immediately prior condition.  The thence caused decrease in the need, as to the amount of kinetic energy that the correlative electron is to then have, is to then result in the just previously stated relative discombobulation.  Such a so-eluded-to back-and-forth wave-tug, that is applied to the Ward-Caucy-based conditions of the here pertinent electron, happens -- as it is to be tugged from initially  moving inward into then immediately moving outward -- of which works to help in causing the tendency of such a released discrete quantum of energy, to then be pushed into that directoral-based holomorphicity, that is in the opposite relative direction from that by which the correlative nucleus of the directly pertinent atom is in.  Such a drop, in and of itself -- in the corresponding energy level of the directly corresponding electron, will then act at such a rate --  by which the specific one-dimensional strand of energy, that is to here be released, will then tend to be brought to the "outskirts" of the Ward-Caucy bounds of the correlative electron, as a fully contracted open strand of kinetic spacial disturbance.  As the said open strand of fully contracted kinetic energy, is to then be in the process of being pushed-out of the correlative electron, the two individually taken zero-norm-state -projections that both work -- in so as to tie the two ends of the initially stated one-dimensional superstring together, in so as to work to form a photon from the now released kinetic energy -- this of which has here been emitted from the so-stated electron, to where the process itself of the Fujikawa Coupling via the mathematical conditions that may be eluded-to by the Green Function, work to help in so as to provide that needed additional thrust, to the said emitted discrete quantum of kinetic energy, -- in so to then work to cause the then formed photon, of which is one discrete quantum of electromagnetic energy, to result in going at the speed of light -- when this is taken in multi-consideration with the directly associated Ward-Caucy-based conditions, that are to here be correlative to the locally proximal state, that may be associated with Snell's Law.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Most Unique Tense Of Noether-Based Current

Any superstring of discrete energy permittivity -- that is not of a tachyonic-based nature, when this is taken over a directly corresponding set of iterations of BRST -- as the so-eluded-to respective superstring is differentiating in a Fourier-based manner, that is over a sequential series of group-related instantons -- is going to be undergoing one tense or another of some sort of genus of Noether-based flow.  Every variation in either the propagation or in the delineation of any given arbitrary superstring, and/or of any given arbitrary orbifold eigenset --  to where this may come together in so as to work to form any variation in either the velocity and/or in the acceleration of any of such respective given arbitrary superstrings, and/or of any of such orbifold eigensets, is going to result in the substringular, as one tense or another of the exhibition of some sort of Noether-based current.  The most unique general genus of a specific sort of Noether-based current -- by which the covariance of any of such a general genus of a Noether-based type of current, exists in such a manner -- to where the inter-relationship of any other orbifold eigenset of phenomenology, that is of any other sort of genus of substringular holonomic substrate -- that is to be both codifferentiable and codeterminable with the initially so-stated general genus of a Noether-based current that I have eluded-to here, is to work to make the general condition of relativity, -- to where this is the general genus of what will here directly correspond to the Fourier-based activity that is related to the speed of electromagnetic energy.  This speed of electromagnetic energy -- of which is also to take into consideration, that covariance that is related to how the speed of light is to vary in any other medium besides a vacuum, as may be typified here as is according to Snell's Law -- may be generically viewed of as the tendency, of the condition, that any phenomenology is effected by both the presence of both the existence and the motion of light, or, that any phenomenology is effected by both the presence of both the existence and the motion of electromagnetic energy.  Here is a simplification that works to describe, in general, what works to help in the formation of that general Noether current -- that is most directly affiliated with the Noether current of light or electromagnetic energy.:  Any orbifold eigenset -- that bears no cohomological-based inhibition towards the formation of those eigenindices -- that work to come together in so as to form the Rham-based pattern of its cohomological-based tracing, will tend to form that Noether-based current, that is most directly associated with the behavior of electromagnetic energy or light.

Part Ten Of The Twelvth Session Of Course 19 -- The Klein Bottle And Orbifold Differentiation

Let me start out with an obvious ansantz -- of which is to here be followed by an explanation of a concept, which will here at that point, be of more of a simpler degree of thought to be understood than otherwise.:  Any given arbitrary imaginary number that is to be multiplied by another given arbitrary imaginary number -- if both of such so-stated imaginary numbers are of a positive imaginary-based nature -- will then result in the computation of what will then be of a negative Real-number-based nature.  Nextly, any given arbitrary Real-number-based value that is to then be multiplied by another given arbitrary Real-number-based value, will then result in the computation of what will here be another value that is of a Real-number-based nature.  Any given arbitrary Kunneth formulation, that would here work to involve the directly corresponding import of a Yukawa-affiliated Yang-Mills light-cone-gauge topology, -- will then result in the Hodge-based adding of the directly associated orbifold eigensets, that are to here be of the so-eluded-to non abelian, or, in other words, of the so-stated Yang-Mills light-cone-gauge topology, to where such a euclidean additive process would then work to acrue to a set of compiled imaginary, or, in other words Njenhuis indices -- since the directly corresponding Yang-Mills symmetry may here be described of as being of an imaginary-norm relation -- to what would here be of a kinematic interaction that is to happen here, towards the directly correlative entropic Real Reimmanian Kaluza-Klein light-cone-gauge-based supersymmetry.  Here.  Let us consider here a set of photons - that, when not scattered, are always to tend to be here of a Yang-Mills light-cone-gauge topology -- that are to quantifically strike and then scatter upon another initially set phenomenology.  The electromagnetic energy, or, in other words, the quantized set of photons -- are to then act in so as to scatter, in what may here be described of as a Calabi-based interaction -- of which will then tend to work in so as to form a Gaussian inter-relation, that is known of as as gauge-transformation. The thus entropic photons, when this is taken immediately after these so-stated photons have been scattered -- will then tend to be perturbated from the initial Yang-Mills topology, into what is to now to be of a Kaluza-Klein light-cone-gauge topology, BUT NOT OF A YAU-EXACT NATURE -- for the initial 384 iterations of group-related instanton, right after the said collision for each individually taken scattered photon is to happen, which is again right after these said photons have acted in so as to bear their correlative Gliosis-based contact, with the multiplicit holonomic substrate that these have collided with.  Even though the overall said scatterered quanta of electromagnetic energy is slowed-up, when it strikes a medium other than a vacuum -- the initially entropic photons are to here initially be sped-up in a flow that is not of a Noether-based nature -- during the said initial 384 iterations of group-related instanton, after these have collided with a metrical-gauge-based Hamiltonian operator, in a Gliosis-based manner.    Immediately after the said 384 initial instantons in which these entropic photons had just sped-up, these respective photons are to then slow-down to a greater scalar amplitude than these had initially sped-up.  Yet, the process of the directly correlative orbifold eigenset -- being put into a "position" in so as to need to "catch-up" with the said entropic photons, as these said scattered photons are being multidirectorally scattered -- works to tend to involve the ironic condition, due in part to the means of the activity of this said "catching-up,"  that scattered light that strikes any medium other than a vacuum will always tend to go slower than light would otherwise travel at, as it is traveling through any of such a medium other than a vacuum, -- as is according to Snell's Law.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some More About The Light-Cone-Gauge

As to the discussion about two sets of superstrings that differentiate covariantly over a given arbitrary Fourier Transformation:  The discribed activity here repeats its mentioned mode in a manner so that it involves a reiterated sequential series of corresponding instantons that strays in a general spot in such a manner so as to not go as a group through a discrete unitary and/or tree-amplitude-based unitized directoral.  The more that a Wilson-Line develops in terms of having more of a basis of unitization among the superstrings that form the said two mentioned substringular groups taken individually -- and especially when such unitization combines the two said groups -- that potentially causes these to form a syncronization that will pull these into a motion that involves a discrete Lagrangian.  Then, such a unitization may spontaneously allign the parity between these related superstrings in such a manner that these would thence converge the arbitrarily related holonomic discharge of substringular field (mini-strings of which form the physical entity of the said field) which, if the Noether-Based flow of  the prior mentioned substringular group catches up with what was earlier the prior mentioned arbitrary tachyonic-based substringular group, this would then need to be on account of what would appertain to a minor spuriousness in the tachyonic scattering of both substringular groups. An example of this, when photons scatter, these are initially tachyonic for relatively few instantons.  Right after that, the said photons that just scattered slow down more than these initially sped up, as according to Snell's Law.  These photons -- in the process -- catch up to the orbifolds in which these are to quantize with in such a manner that photons that travel outside of a vacuum always travel slower On Average than these would travel in a vacuum.  Again, this happens as Snell's Law indicates.  This will be much further discussed in future books that I wrote. 
I will continue with the suspence later!  Sincerley, Samuel Roach.            

A Little As To The Relationship Between Gauge Transformations and the Bette Action

When gauge transformations happen, the Bette Action happens in such a way to where the corresponding superstrings that are here directly related have less of a tendancy to be orientable.  Superstrings that are not only unorientable in the Bette Action, yet, are also unorientable in the Regge Action, become tachyonic until the corelative superstrings that are arbitrarily mentioned here are acted upon to return back to a tense of Noether Flow.  Again, the reason as to why the Bette Action tends to bear a condition of unorientable corresponding superstrings is because of the related shaking of the respective Klein Bottle eigenstates that happens as the superstrings that are consequently within the Neumann region of the said Klein Bottle eigenstate during the respective Kaeler-Metric eigenmetric are also shook by the interaction of the mentioned superstrings that enter the given Klein Bottle eigenstate with the norm-states that exist within the Neumman Ward bounds of the said open-topped parallelopiped entity that helps to physically describe the shape of the said Klein Bottle eigenstate. 
The main functions of the Kaeler-Metric is to both allow for superstrings to regain the discrete metric-gauge that these need to remain as discrete energy permittivity while yet also to allow for their reverse-holomorphically delineated Fadeev-Popov-Trace eigenstates to regain discrete field trajectory metric-gauge so that these may remain as discrete energy impedance.  Metric-Gague in superstrings and also metric-gauge in Fadeev-Popov-Traces is holonomically the topological sway eigenstates that provide the basis of angular momentum relationship that causes the said substringular phenomena to be able to be delineated thru the substrate of space-time-fabric so that the mentioned substringular phenomena may be sufficient enough to move thru the operand of that space so that energy may continue spontaneously.  When both the substringular phenomena that enters the given Klein Bottle eigenstates shakes as well as the holonomic substance of the said Klein Bottle eigenstates shakes as well at the same time, the specific loci where the metric-gauge that produces the proper covariant relationship so that the corresponding substringular phenomena may continue to move thru space spontaneously is pulled and swayed into a slightly broader locus that works to alter the hermitian characteristic of the topological substance of the said substringular phenomena enough so as to alter the homeomorphic Ward conditions of the mini-string that binds the related superstrings to their counterstrings and/or works to alter the relative given arbitrary length of the individual strands of the mini-string that bind between the respective superstrings and their respective counterstrings.  This is simply due to the condition that alterior topological sways that are compounded upon an initial topological sway form a multilateral spin-orbital delineation acts upon a larger Hodge-Basis of a Ward Minkowski surface area.  This is why gauge transformations produce an initial but extremely brief tachyonic conditon in photons that subsequently slows these photons even more than these said photons were directly previously sped up -- according to Snell's Law -- so that the respective photons may "catch-up" to their related orbifolds that these are to quantize with so the said photons that are scattered will always average having a slower velocity than if these were to travel in a vacuum.  If a set of superstrings undergoing a gauge transformation tends to be unorientable in the Regge Action, then, there will be more tachyonic motion in other superstrings that will here arbitrarily convert from Kaluza-Klein to Yang-Mills.     

Some Help As To The Nature Of Scattered Light

When a photon initially strikes a phenomena, it goes from very briefly tachyonic to light-speed to under light speed in such a fashion so that the said photon may be homologous with the orbifold eigenset that it belongs to in the ensuing instantons when it has finished scattering and has been quantized into the beam of electromagnetic energy that it is to be absorbed into.   This happens in such a fashion so as to obey Snell's Law.  --  A beam of electromagnetic energy is propagated slower in any normally conceived medium than it is propagated through a vacuum.  The reason as to why EM energy initially becomes tachyonic when it first strikes another phenomenon is that the light-cone-gauge of the arbitrary EM energy will here initially alter from Yang-Mills to Kaluza-Klein analogous to the function of a shock-absorber, while the environment of the said photons converts its light-cone-gauge topology back into a Yang-Mills topology due to the equal and opposite response to the lack of resistence that the mentioned photon is then going through.  The photons consequently slow to the speed of light while yet slowing to under the speed of light in such a fashion so as to requanize with the orbifold eigensets that are excepting of the spin-orbital momentum, angular momentum, and the various Ward Caucy and Njenhuis characteristics of momentum that are associated with the ability of photons to be absorbed into a beam of light in a quantized manner.  This overall process goes as is according to Snell's Law.
If a photon that scattered never changed temporarily in terms of its light-cone-gauge, then the above wouldn't happen.
If the above didn't happen, then photons would not be able to succesfully be absorbed into beams of light that were homologous enough to allow for the proper requantization.  If that were to happen, light would chaotically scatter in a manner so that heat would not be able to organize to allow for the perpetual existence of mass.
Yet, because of the nature of the Yang-Mills nature of EM-related superstrings, when light scatters, it initially becomes tachyonic due to the initial change into a Kaluza-Klein topology due to the basic nature of the corallary of how springs work.  This is an unchangeable fact just like 1+1 will always be 2.  As photons that have just scatterd are releaved of stress, these will naturally go back to having a Yang-Mills topology due to the fact that physical nature works to obey the laws of inertia.  This activity of the release from the physical stress of scattering causes the described photons to slow down to under the speed of light.  Due to the fact that photons that have arbitrarily just been scattered need to be quantized with orbifold eigensets that are compatible with them, the process of light propagation through something besides a vacuum obeys Snell's Law.  By light, I do not just mean visible light.  --  I mean electromagnetic energy of any sort except that of Kirchoff Radiation.  This is not a eutopia as to how light scattering works, yet, this gives you the general idea.                     
Siincerely,
Sam.                                                      

A Little As To The Nature Of Black-Holes

Hello, my name is Sam. Worm-Holes bear pulsation characteristics that predate the Big-Bang. So, if worm-holes did not exist, then the Big-Bang never happened. Yet, to me it is totally obvious that the Logos struck the core of the Big-Bang from 192 different directions (both sides of 96 different axials) to form discrete reality from indiscrete reality. Space-Time curves. Ultimon Flow is obvious to anyone who can see the see the string theory that they claim to be describing. The fact that Ultimon Flow is real proves that tachyons are infinitelly real. The fact of the above proves that worm-holes are infinitelly real. The fact that Snell's Law is real is provable via the work that I showed yesterday.


                          
What we would normally term of as tachyonic is a set of one or more superstrings that move as a group transversally through a discrete Lagrangian through a discrete enough distance so as to directly interact (in a Gliossi manner) with infrared energy in a manner that goes faster than Noether flow would allow. These must be true in order for reality to exist, period. Sincerely, Sam.                                       

Part One of Sesson Five of Course Six on Fock Space and the Light-Cone-Gauge

Superstrings generally vary in position in one fashion or another by the Planck Length -- although in such a static equilibrium that these described superstrings usually do not move through a discretely directoralized Lagrangian over a sequential series of instantons  at the Planck Length per intanton so as to move at the speed of light -- unless the mentioned superstrings are of EM energy.  Otherwise, such a phenomena is phenomena that involves the bending back and forth of space fabric via a worm-hole, in which the phenomena traveling within a given worm-hole, while in this "hole", only have a Yang-Mills light-cone-gauge topology so as to be able to travel via their kinematically covariant locus up to the speed of light or faster.  You see, anything that is generally considered to us to be a mass always has a Kaluza-Klein light-cone-gauge topology that also has completely Yau-Exact singularities in-between the superstrings that comprise any given mass.  Such a phenomenon cannot go at the speed of light.  (There is no infinite mass).  Yet, if one were to convert the mass' light-cone-gauge topology to Yang-Mills, which is part of what happens when one is translated into a worm-hole (although well over 99 percent of the speed in a worm-hole is due to the back-and-forth bending of space fabric), such of what was translated may travel at the speed of light or faster.  A photon that has initially scattered over the course of relatively few instantons at first has its light-cone-gauge topology converted to Kaluza-Klein as it springs briefly tachyonically, yet a photon as a photon always has only partially Yau-Exact singularities involved directly with them.  (The described singularities are hermitian, yet these singularities vary from on to off of the Real Reimmanian Plane during the course of each instanton.  This is why such an initially scattered photon is not a mass -- yet alone the fact that such a photon does not have infinite mass.  As stated before, after relatively few instantons after a photon has scattered, its light-cone-gauge topology converts back into a Yang-Millls topology at just under the speed of light as it attempts to requantize into one or more beams of EM energy.  The general locus of the orbifold eigenbasis that appertains to any given photon as the described photon scatters is limited in its propagation due to the abelian geometry of the general relative locus, until correlative photons that have just scattered re-enter the mentioned eigenbasis of the associated p field.  The reason for the initial reaction of the photon is based on a similiar concept -- the concept of how and why a shock-absorber works.  The combined effect of the prior described knowledge works to more adequately explain Snell's Law.  (This here would be the why and the how  EM phenomena that travel through a medium other than a vacuum tend to travel at under the speed of light, while EM phenomena that travels through a vacuum travel right at the speed of light (unless the given phenomenon is Kirchoff Radiation).  The interior of a worm-hole is not a vacuum, yet, anything that travels through something like a worm-hole -- that well over 99 percent of its velocity is due to the bending back-and-forth of space fabric -- can, given the conditions, accelerate via its kinematically covariant locus (its actual individual accelleration besides the speed of the bending of space) up to and beyond the speed of light.  Kirchoff Radiation is EM  energy that travels ~6 times light speed, although it does not, in itself, travel in a worm-hole.  I will continue with the suspense later!  God Bless You in the name of Yahweh!  Sincerely, Sam Roach.