A New Ammendment To Session One of Course Eleven On Orbifolds

While a Planck-Related phenomenon is wobbling during an iteration of instanton, the relative wobble allows for the spin-orbitoal momentum or magnetic field fractals of the related Planck-like phenomenon to be orphoganal to the adjacent Planck-like phenomena in four different general substringular-neighborhood loci.  These four "legs" form fields of Planck phenomena that are known of as orbifolds.  This is because the more that you center on a specific locus of Planck-phenomena-related fields, the more that you see a chain of normalized Planck phenomena that are orphoganal by a wobble of ~1.104735878*(10^(-81))I degrees in terms of angular momentum. Yet, the spin and orbit of these Planck-like phenonomena have this wobble occur at four different general locations, thus forming a cross.  This is due to the condition that the Planck-phenomena, throughout one normal cycle of Ultimon Flow, spin in ten dimensions.  When a paranormal or unusual activity happens, these Planck-phenomena may spin in more than ten dimensions.  Up to 96.  This spin jerks the Planck phenomena during that given cycle of Ultimon Flow.  The basis of spatial dimensionality is three dimensions, and, 3*3 = 9.  10 is more than 9.  So, the Planck Phenomena related must be in four different spots via its course of a fractal of magnetic field -- in terms of spin-orbital momentum -- during the corresponding iterations of instanton, in order to allow for the imaginary residue of the Planck phenomena to exchange with Fock Space -- so that the Real residue that directly corresponds to the prior mentioned Imaginary Residue of superstrings, as well as to allow for the condition of the said Imaginary Residue of superstrings, will have the raw holonomic substrate that is viable for the correlative exchanges that are here related. This is so that norm and ground states may recycle in an indistinguishably different manner.  The locant of this is "felt" by the directly prior mentioned general Imaginary Exchange of the directly corresponding superstrings that are here considered in this given arbitrary case, as well as the condition that will here exist as to how the directly corresponding substringular counterstrings will "feel" the effect of what I was just mentioning.  This all happens as the Planck-like phenomena "dance" in such a manner so that these said phenomena may settle, and, thus, this works to allow for the Ultimon Flow to be propagated via the direrctly associated light-cone-gauge-related spring-like motion that happens during BRST.  This exchange is considered Imaginary both because the exchange that I am here discussing is just the end result of many exchanges, and, because the said exchange that is here said to be "Imaginary" is delineated in a back-and-forth manner that is off of the Real Reimmanian plane  -- as opposed to on that given arbitrary plane.

Session 8 Of The Tenth Course Of My String Theory

Let us examine the reiteration contributions of gravitons, gravitinos, tachyonic pulse, dilatons, and dilatinos in respect with the wave-tug of two given arbitrary superstrings that may be mapped in a Laplacian manner via its corresponding world-sheets operands that covariantly interact upon each other, based on a convergent sequential series integration that forms a Fourier-based mapping that consists of taking the individual partial snapshots as to where, how, and when the related world-sheets that appertain here to the mentioned substringular phenomena differentiate over a discrete duration of time in such a manner in that these said world-sheets in this scenario involve both of the mentioned superstrings and their related group semi-attractors -- the attractors of which differentiate in the neighborhood of the two superstringular-related fields that appertain to the fields of strings that form discrete energy permittivity.:
After several iterations of instanton that involve both of the said superstrings in this case, both of the said superstrings of energy permittivity form a logarithmic pattern of expansion and contraction on account of the associated perturbation of the scalar amplitude of the related Polyakov Action eigenmetrics that hence interact with the related Clifford Expansion of the light-cone-gauge that happens per BRST.  This kinematic variaition of parameters in the Ward-Caucy bounds appertaining to the Lorentz-Hamiltonian flow of the affiliated Clifford Expansion eigenoperations forms the semblance of a variable homotopic periphery that has a tendancy of moving in the direction of a hermitian flow in terms of the Ward Neumman alterations that appertain to the kinematic alteration of the Lorentz-operators that influence the associated superstrings in so that the changes that are here applicable to the changes in the mass, time, and length of the mentioned superstrings relative to E.M. bear a Yau-Exact flow in Fourier Translation instead of the mass, time, and length altering in a spurious manner.  The mentioned Polyakov eigenoperations here will consequently wobble from side-to-side during the applicable Imaginary Exchange of Real Residue in so that the coniaxial of the Laplacian-basis of the two said superstrings will be relatively maintained.  In the meantime, the topological integrands of the loci of the Hamiltonian operators that effect the kinematic activities of the said strings will tend to bear a holomorphic field that involves eigenindices which majorize in such a manner so that the said eigenindices will bend the ground conditions of the two superstrings' fields in this case scenario, to where this will add a degree of bilateral Njenhuis tensorism to the Imaginary Ward Caucy conditions of the said strings' holomorphic fields.  This is considering the Dirac function that is associated with the elastic modulae of the said strings holomorphic fields.  On account of this, any smooth torque that is applied to the radial index propagation of each of the two strings holomorphic field generations will redistribute the coniaxial settings of each of the two said superstrings, and this will alter the Lorentz-Four-Contractions effect of relativity upon the said strings in terms of their relativistic velocity and their general limit of velocity.  If the corresponding gravitational particle contributions are Diraced by an acute propagation of group integrands via a kinematic activity that involves a Lagrangian that is delineated thru as is according to a given arbitrary tree-amplitude here, the motion of the two said  covariant superstrings will integrate their motions in a convergent manner over the described related Fourier Transformation thru the whole general operation that I am describing here.  Sam Roach.  

Session Six Of Course Tex

What about substringular singularities?  During the iteration of instanton, Real Reimmanian residue is released and obtained, and, other Real Reimmanian residue that exists in-between superstrings and their counterparts has an Imaginary Exchange that occurs over the duration of BRST that happens during the said iteration of instanton.  The Imaginary Exchange of Real Reimmanian residue may be described by odd functions -- one odd function per individual exchange that exists in-between a substringular first-ordered point particle and its corresponding counterpart.  Odd functions describe activity that is explained in part with Imaginary numbers.  Ultimon Flow mainly happens outside of the duration of instanton on account of the condition that it involves the flow of substringular phenomena when superstrings are not basically at a standstill.  The "time" that happens during Ultimon Flow is imaginary here to us, although this "time" is very actual.  Ultimon Flow outside of the iterating of instanton may be described by odd functions.  Some phenomena that work to describe part of the Ultimon-related time outside of instanton are to be described by singularities which would at first seed to appertain to a degree of relative infinity in terms of the amplitude of some of the corresponding scalars and tensors that are related to the prior mentioned residue.  Phenomena that are smaller than superstrings may be described by singularities that appertain to a degree of relative the infinitessimal in terms of the amplitude of some of the corresponding scalars and tensors that are related to the prior mentioned phenomena.  Yet, the residue of world-sheets and other substringular phenomena that appertain to Ultimon Flow that is outside of the duration of instanton, as well as the description of lengths and other scalars that involve less distance than the Laplacian-mapping of less than: the Planck length (for transversal mapping); and/or the Planck radius (for radial mapping) -- are very Real and very crucial to understand.  The Imaginary Exchange of Real Residue has singularities that apperatin to the relatively infinitessimal in terms of aquainting the Hodge-Indices of the relative bottoms of certain first-ordered point particles that exchange their Hamiltonian-based momentum with the tops of certain other first-ordered point particles.  These condtions involve numbers, that, in terms of the Dirac operations that include the Clifford-Expansion activity that often includes what happens during Polyakov Action eigenmetrics which occur during BRST, may be described by odd functions.  This is due to the condition that the very indiscretely small and the indiscretely large involve alterations in certain Ward-norm-conditions that are respectively either above the scalar range of "normal" computions or below the range of "normal" computation.  Activity that happens off of the Real Plane involves Ward tensors that are to be Imaginarily computated.  The very small work to define the very large, and thus the singularities and odd functions of the very small work to form not only our normal globally distinguishable space, yet, this acitivity also works to describe the singularities and odd functions of the very large.  We exist in a world that observes energy based on Planck phenomena-related phenomena to our perception.  The norm gradients that integrate in-between  infinitessimal and  infinite singularities, as well as the norm gradients that integrate between Njenhuis tensors, to define the workings of the globally distinguishable.   Sam.       

Part Two Of The Second Session Of Course Ten

As the superstrings iterate, the light-cone-gauge quanta that I described in the first part of this session a while ago act as reins that cause the Planck phenomena to dance into their ensuing iteration.  The spin, orbital, and transversal responses of the corresponding Planck phenomena send mini-stringular impulses that cause the Imaginary Exchange of the said related substrings.  The Imaginary Exchange of the substrings mentioned here push the light-cone-gauge quanta inward to spring the substringular into the process of Ultimon Flow-based action as the light-cone-gauge eigenstates that I am here reffering to spring outward.  This happens in such a manner so that the light-cone-gauge-related Fock Space gears the positive-norm-spaces to form ghost anomalies at the points where the said superstrings and their fields were.  As ghost anomalies have formed, the negative-norm-spaces are pulled orphoganally by the positive-norm-states so as to annhilate the ghosts that had recently formed.  This produces residue in the form of the dilatons and the dilatinos that quantize to form basic quantum of gravitational particles.  I will continue with the suspence by typing out the third session of this course soon.  You have a phenomenal day!  Sincerely, Samuel David Roach.    

Some Knowledge About The Bette Action

During the duration in which the Imaginary Exchange of Real Residue happens, both the Polyakov Action and the Bette Action happen.  The Polyakov Action is the reverse contraction of a given superstring that matches the degree in which the here given superstring is kept from full Lorentz-Four-Contraction.  The Bette Action is the Laplacian geometric condition in which the individual substringular fields, in the form of mini-string segments, that exist in-between a given arbitrary superstring of discrete energy permittivity and its correspondint counterpart, are attempted to bear both a homeomorphic wave pattern in-between the two just mentioned topological stringular phenomena all along the Laplacian mapped contour around (for 2-d strings) or all across the Laplacian mapped contour across (for 1-d strings) the contour that binds a superstring and its counterpart. This is as well as the condition of the superstrings in relation to their counterparts bearing an equal topological length along the Laplacian mapping of the mini-string segments that are here to interconnect the said superstring and its corresponding substringular counterpart.  The conditon of a superstring and its Laplacian-Based forward holomorphically placed counterpart bearing mini-string that interconnects these that are equal in the scalar that is relating to the topologically mapped distance that the said mini-string segments have in-between their corresponding superstrings and their counterparts is called an eigenconditon of the Grassman Constant.  If either the topological Laplacian mapping of the said segments that are here used to interconnect the said superstrings and their counterparts, as considered over each potential stretch eigenconditon of an arbitrary given superstring and its counterpart, is homeomorphic over the course of the Polyakov Action (which is during the Bette Action), and/or, if -- during the individual segments of the said potential stretching of any particular superstring, when taken as covariantly discrete integrands of correspondence with the related Lorentz-Four-Contractions that are arbitrarily related here in a specifically given scenario, bear an equally mapped scalar in terms of the length of the said contour -- (The Grassman Constant applies to the consistency of having the same topologically mapped distance between a said superstring and its corresponding counterstring over the duration and activity of the Polyakov Action) -- , then, the related superstring(s) are said to be orientable over the course of the described Bette Action.  I will elaborate later.  Got to run!  Sam.  

String Theory Glossary For Courses Nine And Ten

1)  Real residue -- Substringular residue that happens during BRST.

2)  Imaginary Residue -- Substringular residue that happens during the Ultimon Flow duration that exists in-between the individual metrics in which instanton is happening.

3)  BRST -- Substringular activity that happens during the neighborhood of the activity of instanton.  This duration includes when the Bette Action and the Polyakov Action are occuring, yet, it does not include when the Regge Action and/or when the Kaeler Metric are happening during any given arbitrary duration of instanton.
 
4)  Iteration -- The activity of Globally distinguishable noticeable time in which instanton is occuring.

5)  Ultimon "Time" -- That set of covariant metrics that occur in-between the individual durations in which instanton is transpiring.

6)  Real Exchange -- The substringular exchange that happens on the Real Reimmanian Plane.

7)  Imaginary Exchange -- The substringular exchange that happens off of the Real Reimmanian Plane.

8)  The Core Of BRST -- The Real Residue that is undergoing recycling during the Imaginary Exhange that is operating during the duration that I previously described as BRST.

9)  The Light-Cone-Gauge -- The Laplacian-Based connections in-between Planck-Related phenomena and their corresponding forward-holomorphically delineated superstrings.

10)  Fock Space -- Superstringular phenomena that exists besides substrings, counterstrings, Planck-Related phenomena, substringular encoders, substringular encoder counterparts, and the Main-Heterotic-Stringular-Fabric.

11)  Gravity -- As a weaker force than the electromotive force, while yet still being a relatively stronger force than spontaneous radioactive decay, gravity is that force that pulls phenomena into a tangible interactive order on account of the Ricci Scalar that is physically caused by the Rarita Structure.

12)  Dilatons -- Transversal indices that quantize to form transversal gravitational particles.  These dilatons are formed by the activity of positive-norm-states that are "scooped-off" of world-sheets via the activity of negative-norm-states colliding with the fields of the said positive-norm-states in a manner that is directoralized in such a fashion so as to not bear a Gaussian-Norm Hamiltonian-Basis in terms of the related Gliossi scattering that is being described here.

13)  Negative-Norm-States -- Those indices of Campbell-Projections that are latent in Fock Space that "scrape-away" Gliossi-Sherk-Olive indices, on account of their relatively reverse-holomorphic directoralization  This happens in order to convert the excess sub-spaces of world-sheets into those dilatons and dilatinos that are brought off of the initially implied Real Reimmanian Plane so that gravitational particles may form.  The fields formed by the reverse fractal of such an activity that the Fourier-Based motion of such negative-norm-states causes allows for any needed exchange between Gliossi-Sherk-Olive-Ghosts and Neilson-Kollosh-Ghosts, so that substringular regions may "clear-up" some room for the necessary activity of superstrings and gravitational particles that must occur so that substringular phenomena may spontaneously and continuously differentiate kinematically over the sequential series of multiplicit covariant Fourier Transforms.  Neilson-Kollosh-Ghost indices are scattered by a similar activity of fields that are similar to negative-norm-states, except that the activity that happens here is off of the relative Real Reimmanian Plane.  

14)  Positive-Norm-States -- Those indices of Campbell-Projections that are latent in Fock Space that produce Gliossi-Sherk-Olive indices via the settling of their multiplicit fields on account of their intrinsic forward-holomorphic Fourier-Based directoralization.  Neilson-Kollosh-Ghosts are formed by indices of similar norm-state projections, except that the activity of such indicated indices here is kinematically operated off of the relative Real Reimmanian Plane.

15)  Dilatinos -- Spin-Orbital indices that are formed by the scattering of positive-norm-states by negative-norm-states that quantize to form the particle-basis of gravitinos.

  16)  Gravitons -- The particle-basis of transversally discrete physical units of gravity.

17)  Gravitinos -- The particle-basis of spin-orbitally discrete physical units of gravity.    

       

Session 15 Of Course Nine

The light-cone-gauge multiplicitly exists between Planck phenomena and superstrings.  The light-cone-gauge corresponding to one-dimensional superstrings consists of five mini-string segments that are in-between an arbitrarily corelative Planck-like phenomena ansd its corresponding one-dimensional fermionic string.  With a bosonic string, there are ten mini-string segments in-between the corelative Planck phenomena and its two-dimensional bosonic superstring.  When a one-dimensional superstring closes via the Fujikawa Coupling as may be mathematically described when using the Greene function, the five doubled up milni-string segments unravel and reconnect to form ten mini-string segments that connect homogeneously along the newly formed two-dimensional bosonic string.  So, when a two-dimensional bosonic superstring undergoes such a Yakawa Coupling via the Greene function to open to form a one-dimensional fermionic string, the ten mini-string segments mentionesd double-up to form five mini-string segments after the ten mini-string segments that were previously mentioned are released and ravled to reconnect in a homogeneous manner.  These switches in mini-string happen during iteration or instanton with the help of gauge bosons.  Gauge bosons are an example of two-dimensional superstrings that are larger than superstrings.  Gauge Bosons spin and roll to allign the light-cone-gauge during the activity that occurs during BRST.  BRST is when the Imaginary exchange of Real residue happens among superstrings that are discrete energy permittivity and their counterparts.  (The counterparts of such mentioned superstrings act as a substrate for the said strings.)  The gauge bosons act as "light-switches" that activate the other heterotic strings.  I will discuss what I mean by that in future courses.  As the gauge bosons counterspin and counter-roll, the corresponding activity levers thru space in a hyperbollic manner so that the other heterotic superstrings are able to spontaneously open when necessary so that their counterstrings may retie as one-dimensional superstrings during certain circumstances, and also so that other phenomena that is directly attached to the corelative substringular encoders may undergo the proper retying during the metric in-between instantons when such retying is prominent.     

More About the Activity of the Light-Cone-Gauge

During BRST, which is the main part of a duration that is known of as instanton, superstrings and their counterparts go thru a gauge-metric that I call the Imaginary Exchange of Real Residue.  During this activity, the substringular fields, appertaining to superstings that are discrete units of energy permittivity, that interconnect superstrings with their counterparts -- the field eigenstates which are in the form of mini-string segments -- cause a wobbling motion that initially moves the counterparts of arbitrary superstrings in the forward holomorphic direction while counter-wobbling the corresponding superstrings in that same given forward holomorphic direction.  Such a gauge-metric consequently moves the given corresponding superstrings to wobble back in the associated reverse holomorphic direction while counter-wobbling the corresponding superstrings in the corresponding reverse holomorphic direction.  This happens while the Polyakov Action and the Bette Action are taking place.           
During the simultaneous activities of the Polyakov Action and the Bette Action, the associated superstrings and their corresponding counterstrings alter in scalar relative size via the increase of substringular wave or mini-string segment scalar increase in such a way that the associated superstrings and their corresponding counterstrings largen just enough to be at the length (for 1D strings) or circumference (for 2D strings) that corresponds to how small the associated Lorentz-Four-Contractions are.  As an example, if the Lorentz-Four-Contraction upon a given superstring is zero, then, the associated 1D strings increase during BRST in length by a factor of 3*10^8.  Or, as another example, if the Lorentz-Four-Contraction upon a given 2D string is zero, then the circumference of the associated superstrings increases by a factor of 3*10^8.  This is done with a maintainence of homotopy on account of mini-string being brought into the Gliossi field of where the mentioned superstrings and their counterstrings are at.  Once the corresponding superstirngs and their counterstrings have wobbled back into their original general locus via the reverse holomorphic wobbling of the associated counterstrings counter-wobbling the corresponding superstrings, the effect of this activity springs superstrings and their counterstrings into the Regge Action while then going into Ultimon Flow directly afterward, if their is no Kaeler-Metric during the course of the associated eigenstate of instanton.  If Kaeler-Metric is to happen during a particular arbitrary eigenstate of instanton, then, immediately after BRST, the mentioned superstrings initially enter their corresponding Klein Bottle eigenstate-like phenomenon for half of the rest of instanton -- the superstings of which in the process recontracting to the size that these had directly before these had expanded on account of the Polyakov Action, due to the differential geometry of the norm-states that exist in the given Klein Bottle eigenstates -- while then the superstrings go into the Regge Slope via the Regge Action for the other half of the rest of the arbitrary given eigenstate of instanton.  What we tend to notice in terms of time is instanton, or, more specifically, the BRST portion of instanton.  BRST happens for
6hbar time, while the rest of instanton happens for ((2pi hbar)-(6hbar)) time.  We only tend to notice instanton on account of the condition that superstrings are at a relatively organized standstill during the individual eigenstates of instanton.  By far though, most substringular activity happens in-between the individual eigenstates of instantons.  The Klein Bottle eigenstates are organized to be at the proper location on account of:  1) The abelian propagation of the Wick Action that is tensorically directoralized via the harmonics of wave-tug of the corresponding Schwinger Indices that travel as vibrational eigenstates along the Rarita Structure.  2) The corresponding abelian propagation of the Landau-Gisner-Acion upon the associated  Douboult cohomological section of the Rarita Structure known of as the field where the Fischler-Suskind-Mechanism happens. 3) The abelin nature of the Higgs Action eigenstates upon their associated Klein Bottle eigenstates toward the resultant of the hermitian Ward path that moves in the path of most resistance to the general location where the Kaeler-Metric is to happen.  The combined activities mentioned in the prior are what cause the proper inter-relations that allow for the correct distributions of Klein Bottle eigenstates with their corresponding superstrings so that the superstrings that need metric-gauge -- as well as the superstrings that may also then need to change in light-cone-gauge topology --  may be properly organized so that Gaussian Transformations may happen appropriately.  Sam Roach.      

Course 9, First Course of Fock Space and the Light-Cone-Gauge, Session 12

How do Planck Phenomena propagate?:   Strings are in iteration in the following arbitrary case scenario.  Imaginary exchange as described by an odd function happens as real residue is given off here and received.  This means that the relative bottoms of the here mentioned superstrings are exchanged with the corresponding relative tops of the respective substringular counterparts.  (The superstrings & their counterparts are now decompactified by a factor of one to 3*10^8.)  This prior activity rasises the stringualr counterparts and moves these "down" closer to the prior mentioned superstrings.  The slack here causes the discussed bottom of the substringular counterparts to exchange with the said tops of the corresponding superstrings (reciprocal imaginary exchange).  The prior activity lifts the superstrings (not to be confused with their counterparts) and moves these down closer to their corresponding Planck Phenomena.  The Planck Phenomena stays relatively stationary in the meanwhile -- when not including the wobble of the said Planck Phenomena.  This motion that I have just described contracts the light-cone-gauge like a spring, causing the ensuing Ultimon Flow.  This springing flaps the angular momentum of indices of the said Planck Phenomena in an anharmonic/harmonic cycle that flaps just enough to allow Ultimon Flow, like a paint stirrer twitches then flapped.  The twists in the light-cone-gauge eigenstates that are related to what I just mentioned bears gauge-metrics that help determine whether or not the superstring travel at any given velocity and/or tensorically based speed or not. (The "tensorically based speed" would be a velocity that is based on the directoralization of a tree amplitude.)  A full twist in the fabric of the light-cone-gauge allows for a relatively "infinite" speed, such as the amplitude of phenomena displacement that happens during Ultimon Fllow,  while any twist quotient in-between allows for any speed of the superstrings in-between, since tachyonic motion may redistribute phenomena to basically any other location in just one sequential series of instantons.  Such a displacement that is derived in-between the Real Reimmanian duration that exists from one instanton to the next one may redistribute phenomena as such on account that Ultimon Flow is the Imaginary based flow that cycles the Ultimon in-between two consecutive Real Based instantons.  These mentioned twists are never entangled when unfrayed, yet, the twists are in the individual fabric of the five-quantum-based and ten-quantum-based first-ordered light-cone-gauge eigenstates that are associated with one-dimensional and two-dimensional superstrings respectively.  Two-Dimensional superstrings may influence one-dimensional strings to have their light-cone-gauge first-order-based quanta to twist to an arbitrary proscribed extent and vice                                                        versa.                                                                                                                                                      
I will continue with the suspence later.  Expect a lot of posts soon now that I have my time freed up and my computer is working better now!  God Bless.  Samuel David Roach.                                                                            

Session 10 of Course 9

Hello there world, this is Sam Roach here!  I hope that you enjoy the ensuing post!
Here's how the exchange between Real and Fock Spaces is Imaginary between Real and Fock superstrings:  As an example, the bottom of the bottom of point particles of Real-Based superstrings exchanges a little bit of mini-string to the top of the bottom point particles of a Fock strings point particles in a sinusoidal manner, lifting the Fock strings mentioned to a certain gauged distance.  This also goes for all of the first-ordered point particles that comprise Real and Fock-based superstrings. The superstrings then lower due to the added phenomena.  Once this is done, the botom of the bottom mentioned Fock string's point particles exchanges a little bit of mini-string to the top of the bottom point particles of Real strings in a sinusoidal manner, raising the Real strings to the same extent that the Fock strings were originally raised.  Agian, this also goes for all of the first-ordered point particles that comprise the arbitrarily mentioned superstirngs.  The strings then lower due to the added phenomena that I have been describing here.  This happens with superstrings during the course of what is known as BRST.  This helps settle the "dance" of the Planc phenomena that these strings are connected to by light-cone-gauge eigenstates via mini-string segments.  This exchange is Imaginary since the mini-string segments' ( exchange that happens between the point particles of the Real and Fock stringular counterparts) happens at the opposite ends of the point particles, causing the exchange to be off of the Real Reimmanian plane that is subtended between the point particles of the Real and Fock Strings.  Before the Imaginary Exchange, the Real Reimmanian-based superstrings' (as compared with their counterparts) point particles are just over half condensed oscillation, and the Fock strings' point particles are just under half full.  During the first Imaginary exchange under the condition of a superconformally invariant setting, both the Real and the Fock-related superstrings are half condensed oscillation.  After the Imaginary exchange of the given iteration (which is the duration during instanton),  the Real strings' point particles are just over half conesnsed oscillation, and, the Fock strings' point particles are just under half full.  So, even though a first-ordered point particle always has the same total locus of volume, the degree to which it is filled is defined by the density of the mini-string that comprises a said first-ordered point particle.  For instance, a just over half-filled point particle of the first order is just over 50 percent of the maximum density that second-ordered point particles -- in the context of mini-string -- can possibly fill the associated volume that a first-ordered point particle tends to have.  Yet, a just under half-filled point particles of the first order is just under 50 percent of the maximum density that second-ordered point particles -- in the context of mini-string -- can possibly fill the associated volume that a first-ordered point particle tends to have.  The relatively Laplacian-based degree of what I call point-fill here refers to a non-time oriented perspective as to the density of mini-string while it exists in the Neumman bounds of the locus where a first-ordered point particle is existing ( the density of such in one "snapshot" of duration).