Showing posts with label Collosh ghost anomalies. Show all posts
Showing posts with label Collosh ghost anomalies. Show all posts

Wednesday, September 19, 2012

A Little Extra About Ghost Anomalies

To be very brief yet concise -- since whenever a superstringular phenomenon moves, it produces a physical memory of where it had been, superstringular pheneomena are always producing ghost anomalies indirectly per sequential series of instantons.  This is in part do to the condition that world-sheets are the physical mapping of where superstringular phenomena has been, and, world-sheets have partial formations that integrate over the course of any given arbitrary sequential series of instantons so as to produce evidence of the history of substringular phenomena -- such evidence of which is indicated by the here caused existence of ghost anomalies.  The kinematics that consequently is caused indirectly by the existence of ghost anomalies forms an equal and opposite reaction in terms of norm-related Fourier conditions that works in the relativistically equal and opposite diretoralization so as to scatter the corresponding given arbitrary ghost anomalies.  So, whenever there is motion, there is creation and destruction -- as may be depicted here by the consequent creation and destruction of ghost anomalies.  Ghost anomalies also indirectly share eigenstate indices with other ghost-related phenomena in order to allow such a physical holonomic balance, in such a manner so that there is enough room allowed for those kinematic inter-relations that allow for the continuation and perpetuation of energy -- so that energy and reality may continue to exist.  Sincerely, Sam Roach.  

Wednesday, June 20, 2012

Part Two Of The 14th Session Of Course 10

To go back from where I left off, point commutators form Fock Space.  The propagation of ghost anomalies forming, as well as the condition of ghost anomalies becoming undone, helps to pull the associated superstrings through their world-sheets.  Yet, the related activity just mentioned causes the potential for tadpoles, these tadpoles of which are anharmonically-based metrical point commutator fields that strike the center-state of the corresponding superstrings at 45 degrees to both positive and negative-norm-states.  Yet, the condition that ghost anomalies always will happen is due to the large number and density of reverse-holomorphic norm-states,as well as the condition that ghost anomalies will always happen du to the large number and density of forward-holomorphic norm-states.  Such phenomena going through such associated activity works to create a balance that works to prevent damage to space-time-fabric on account of the fact that freeing up room in the substringular allows for the ample distribution and motion of superstring-related phenomena so that activity and thus energy may exist.  Tadpoles need to be utilized quite often over billions of years to have much effect.  The longer that a tori-sector-region (a layer of reality of one parallel universe) has been acitivated, the more that there is a potential that there is for tadpoles to have a significant effect.  A balance among both the frequency and the scattering away of ghost anomalies is a condition that works to determine both the creation of and the attribution that is here due to the existence and the time-related activity of tadpoles. 

Sunday, May 6, 2012

The Third Session Of Course Ten

Stringular fields of one-dimensional superstrings are disc-like, and stringular fields of two-dimensional fields are spherical-like.  The light-cone-gauge eigenstates intaeract with substringular fields -- and are joined together with these.  Superstrings tend to be centered in their substringular fields.  World-Sheets are enacted upon by these fields by acting conformally invariant with the Ward-Caucy boundaries and the other related Ward conditions of the radial and transversal differentiation of the fileds of one and two-dimensional substringular fields.  The corresponding ghost anomalies that form during the Fourier-metric differentiation of the said substringular fields form as core stringular ghost fields that are surrounded by core stringular ghost anomailies.  The ghost anhilators that form disperse the ghost anomalies by normalizing the point commutator fields that are distributed by the related ghost anomalies.  The said ghost anomalies that are thus formed are due to the differentiation of the said corresponding world-sheets upon the positive-norm-states that surround the related superstrings, as well as the related stringular fields.  The ghost annhilators are the negative-norm-states that happen to move in the reverse-holomorphic directoralization of the respective positive-norm-states.  Positivt-Norm-States are comprised of the point commutator orientation that I have discussed before, and, these here are near the respective superstrings and their respective substringular fileds that are in the general direction -- as may be derived based on the norm-conditions that correspond between these both during the same general metric.  The negative-norm-states are comprised of the same general type of phenomenology as positive-norm-states, except, these move in the reverse holomorphicity (reminder).  The zero-norm-states are the loose point commutators that work to open two-dimensional superstrings at certain times, while these at other times work to close one-dimensional superstrings.  Every point commutator is a first-ordered-point-particle that is not in either a superstring, a counterstring, or a Fadeev-Popov-Related-Type-Ghost when considered during BRST in their respective world-tubes.

Wednesday, May 2, 2012

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.    

Thursday, April 12, 2012

Part Two Of Course Two Of Course Nine

The operator that I mentioned near the end of the first part of session two is, in their respective cases, one of the following:  a covariant organization of directly affiliated phenomena that are either zero-norm-states,  Hausendorf-Projections,  Campbell-Hausendorf-Projections,  Campbell-Projections, in some cases, simply the mini-string that binds the relative "up" and the relative "down" of  norm-states, or, in other cases, a combination of the just prior types of phenomena.  Such respective types of operators work to pull the scattered norm-states in such a manner so that the ghost anomalies (in some cases) or the just annhilated ghost anomalies (in other cases) may manuver in an appropriate manner around the direct field density of either the two-d fields of one-d superstrings or the 3-d fields of 2-d superstrings.  This helps to describe how -- to an extent -- norm-states work to form either ghost anomalies or to scatter these ghost anomalies so that gravitational particles may have a basis of formation.  I will continue with the third part of this session later!
Hope in anticipation for the suspence!  Sam Roach.    

Wednesday, April 11, 2012

Session Two Of Course Ten, Part One

Here's how light-cone-gauge eigenstates interact with Fock Space that is proximal to an individual given arbitrary first-ordered light-cone-gauge eigenstate.  A first-ordered-light-cone-gauge eigenstate differentiates transversally, orbitally, and spin-orbitally during the course of instanton, and, also during Ultimon Flow.  The said light-cone-gauge eigenstate differentiation effects its surroundings.  The directly associated Fock Space Ward-Neumman-Based region that surrounds the said eigenstate is most directly effected by the differentiation of the sum of the second-ordered-light-cone-gauge eigenstates that comprise the corresponding first-ordered-light-cone-gauge eigenstate during the course of the given arbitrary iteration of instanton that is here being discussed in this case.  The said sum of the second-ordered-light-cone-gauge eigenstates also effect the activities that occur during the ensuing Ultimon Flow to a certain extent -- since the sum of directly associated second-ordered-light-cone-gauge eigenstates forms a first-orderd-light-cone-gauge eigenstate.  This Fock Space that is most directly effected by the said first-ordered-eigenstate may be termed of as light-cone-gauge-related-Fock Space.  Light-Cone-Gauge transversal momentum produces a light-cone-gauge-transversal-based Fock Space.  Light-Cone-Gauge-related orbital momentum produces a light-cone-gauge orbital Fock Space.  Light-Cone-Gauge spin-related momentum produces a light-cone-gauge spin Fock Space.  The differentiation of light-cone-gauge transversal-based Fock Space and the differentiation of light-cone-gauge orbital-based Fock Space and the differentiation of light-cone-gauge spin-based Fock Space provides a multiplicitly-based type of operator for positive-norm spaces so as to form ghost anomalies, while the said general type of differentiation at a different general locus of the light-cone-gauge produces a multiplicitly-based type of operator for negative-norm spaces so as to form phenomena that annhilates ghost anomalies.  The residue of annhilated ghost anomalies works to form those phenomena that indirectly are used to form the phenomena of gravitational particles.  I will continue with the second part of this session later!  
Sincerely, Sam Roach.

Thursday, June 9, 2011

A Little Bit About Ghost Anomalies

The ghost anomalies that are created and not elliminated from within the Real Reimmanian Plane of an arbitrary substringular setting often exchange places in terms of relative Laplacian settings with the Neilson-Collosh ghost anomalies that are Njenhuis to the arbitrary mentioned Real Reimmanian Plane.
Generally, the ghosts that are formed in the Real mentioned plane are elliminated by reverse-holomorphic norm-states that scatter the configurations of general physical memory that are temporarily formed by forward-holomorphic norm-states.  The same general tendancy exists also for the Neilson-Collosh ghosts that are formed in the corresponingly Njenhuis Plane where gravitational particles differentiate through the multiplicit Fourier-based Lagrangians that are necessary for the continued existence of the Ricci Scalar that exists due to the activity of the Rarita Structure.  Yet, when ghost anomalies that are covariantly Njenhuis relative to one another, as is the case for regular substringular ghosts versus their corresponding gravitationally-based ghosts, are not spontaneously elliminated so that there may be enough freedom of motion for superstrings to differentiate in a Fourier manner, these relatively Njenhuis ghosts exchange where these differentiate in terms of the norm-based Ricci Scalar Njenhuis Laplacian settings in such a manner so that such arbitrary ghost anomalies may be scattered so that there may be sufficient room for superstrings to differentiate over a sequential series of Fourier Translation.  Although the conditions of such a displacement is like a snapshot of covariant displacement, the activity of such a displacement is a relatively brief Fourier Transformation that is needed.  The scattering of ghost anomalies facilitates the motion of Hausendorf Projections to differentiate through the multiplicit Fourier Lagrangians that are necessary for the activity of an arbitrary Hausendorf Projection that is known as the Wick Action.  The Wick Action is created by the metrical activity of gluons.  The Wick Action indirectly causes the type of translation of the Higgs Action that is needed so that the Klein Bottle may be displaced so that the Kaeler-Metric may happen so that Gaussian Transformations may happen.  The activity of Gaussian Transformations thence allows for the spontaneous alterations of norm-conditions that are necessary so that Fourier Transformatons may be kinematic in their loci, and the prior allows for the necessary interchanges that allow for energy to be perpetual period.  Also, Gaussian Transformations are necessary for superstrings and their field trajectories to retain their respectice discrete energy permittivity and discrete energy impedance.  Gauge-Transformations, which are a fundamental form of a Gaussian Transformations, are needed in order for the switching of abelian conditions that are necessary in order for the scattering of electromagnetic energy to continue in any way that is feasible given the present conditons of space-time fabric.  Gauge-Transformations are also neede for the existence of entropy, and entropy is needed in order for there to be any change in physical states.
Thank you for your time.  Sincerely, Sam Roach.