7) Particles that work to comprise, for instance, nucleons and electrons -- such as quarks and leptons.
6) Superstrings.
5) First-Ordered point particles.
4) Second-Ordered point particles.
3) Third-Ordered point particles.
2) Sub-Mini-String (The ultimate fractal of pressurized vacuum).
1) The Logos.
Showing posts with label sub-mini-string. Show all posts
Showing posts with label sub-mini-string. Show all posts
Saturday, December 28, 2013
Wednesday, March 20, 2013
The Importance of Point Particles to the Existence of Superstrings
In order for superstrings to be able to differentiate and interchange kinematically, there must be point particles that are smaller than these discussed superstrings. A superstring has a length, for 1-D strings, and a circumference, for 2-D strings, of 3*10^(-35) meters in the globally distinguishable. When in a totally contracted state, such a scalar is 10^(-43) meters. A first-ordered-point-particle has a diameter of 10^(-86) meters in the substringular when including the Gliossi Field that is directly associated and thus comprises the said point particle. First-Ordered-Point-Particles are comprised of the substance of the field of superstrings, or, in other words, mini-strings. Mini-String is comprised of second-ordered-point-particles that exist adjacent to each other in exterialy bound "chains" of phenomena that are interconnected by third-ordered-point particles that are bound by sub-mini-string. Second-Ordered-Point-Particles are 10^(-129) meters in diameter in the substringular, third-ordered-point-particles are 10^(-387) meters in diameter in the substringular, and sub-mini-string is 10^(-1161) meters in diameter in the substringular. Sub-Mini-String is the smallest phenomena that is a thing while yet also a gauge-action. Third-Ordered-Point-Particles only exist where there are second-ordered-point-particles. Not only does sub-mini-string bind third-ordered-point-particles together, yet these also work to interconnect the second-ordered-point-particles that comprise mini-string. A physical entity that is smaller than a superstring is termed to be a gauge-action. So how does such a tying of fabric rety while yet maintaining homotopy? The "space-hole" is what I call the duration right before Instanton-Quaternionic-Impulse-Mode, which is right before instanton, which is when homotopy just begins to undue to allow any essential retying of string, yet, to such a minor amount that homotopy during successive instantons is maintained except for when it is frayed in a black-hole. Such a resewing of substringular phenomena is brought back into a multiplicitly discrete homotopy due to the pressure that is impelled upon adjacent superstrings due to the equal and opposite wave-tug of point-particles that acts Gliossi upon the said superstrings to just enough of an extent so as to snap the temporarily untying topology described back into a unified multiplicit homotopic topology. There must be phenomenology smaller than superstring in order for their to be the holonomic subtrate that works to form substringular fields. Sincerely, Sam Roach
Wednesday, December 5, 2012
Another Major Force
The strongest when considered overall, yet, the weakest when taken in a locally sub-Gliossi manner, force, would be that fractal of pressurized vacuum that holds sub-mini-string together in such a manner so that third-ordered-point-particles -- and thus, second-ordered-point-particles -- may be held together. Such a force thereby works in such a manner in so that mini-string may keep together, so that the fields of superstrings may remain fractally vigilant. The ability of the fractal strength of substringular fields works to keep first-ordered-point-particles and also decompacitified substringular fields together so that superstrings, and thus, phenomena, may remain in tact.
Sincerely,
Samuel David Roach.
Sincerely,
Samuel David Roach.
Wednesday, August 22, 2012
Point particles
The Importance of Point Particles to the Existence of Superstrings
In order for superstrings to be able to differentiate and interchange kinematically, there must be point particles that are smaller than these discussed superstrings. A superstring has a length, for 1-D strings, and a circumference, for 2-D strings, of 3*10^(-35) meters in the globally distinguishable. When in a totally contracted state, such a scalar is 10^(-43) meters. A first-ordered-point-particle has a diameter of 10^(-86) meters in the substringular when including the Gliossi Field that is directly associated and thus comprises the said point particle. First-Ordered-Point-Particles are comprised of the substance of the field of superstrings, or, in other words, mini-strings. Mini-String is comprised of second-ordered-point-particles that exist adjacent to each other in exterialy bound "chains" of phenomena that are interconnected by third-ordered-point particles that are bound by sub-mini-string. Second-Ordered-Point-Particles are 10^(-129) meters in diameter in the substringular, third-ordered-point-particles are 10^(-384) meters in diameter in the substringular, and sub-mini-string is 10^(-1152) meters in diameter in the substringular. Sub-Mini-String is the smallest phenomena that is a thing while yet also a gauge-action. Third-Ordered-Point-Particles only exist where there are second-ordered-point-particles. Not only does sub-mini-string bind third-ordered-point-particles together, yet these also work to interconnect the second-ordered-point-particles that comprise mini-string. A physical entity that is smaller than a superstring is termed to be a gauge-action. So how does such a tying of fabric rety while yet maintaining homotopy? The "space-hole" is what I call the duration right before Instanton-Quaternionic-Impulse-Mode, which is right before instanton, which is when homotopy just begins to undue to allow any essential retying of string, yet, to such a minor amount that homotopy during successive instantons is maintained except for when it is frayed in a black-hole. Such a resewing of substringular phenomena is brought back into a multiplicitly discrete homotopy due to the pressure that is impelled upon adjacent superstrings due to the equal and opposite wave-tug of point-particles that acts Gliossi upon the said superstrings to just enough of an extent so as to snap the temporarily untying topology described back into a unified multiplicit homotopic topology.
Monday, December 19, 2011
Here Is Some Knowledge To Help You To Better Understand Sub-Mini-String
Sub-Mini-String is what interconnects both third-ordered-point-particles to each other as well so as to interconnect second-ordererd-point-particles into the type of mini-string that forms the fields that are exhibited by superstringular phenomena. First-Ordered-Point-Particles are formed by the "yarning" of mini-string into the various forms of compactifications that allow for the respective various forms of first-ordered-point-particles that exist in the arena of space-time-fabric.
Sub-Mini-String segments bind via an extreme fractal example of a pressurized vacuum. Ideally, one would think that sub-mini-string segments would be flushly homeomorphically cylindrical. Yet, the ends of the segments of sub-mini-string are not necessarily a fractal of cross-sectional orientafolds. Often, either end and/or both ends of sub-mini-string segments are conically angled by up to 11.25 conical degrees if one were to observe such a conical angling at such a close range that a given arbitrary sub-mini-string segment would here appear to be three-dimensional. Such an angling may be singularized, trivially isomorphic when one considers both ends of such a mentionable segment, or non-trivially isomorphic when one considers both ends of such a mentionable segment. So, when such a said segment is non-trivially isomorphic at its maximum conical slanting at both ends, the overall conical angling difference would, in under a Laplacian condition, be a 22.5 degree difference. This coincides with the condition that a Higgs Action eigenstate subtends to an angling of 22.5 degrees to the relative left of a relatively straight up and down subtending when a Klein Bottle eigenstate is to move holomorphically and that the same arbitrary Higgs Action eigenstate subtends to an angling of 22.5 degrees to the relative right from a relatively straight up and down subtending when the respective Klein Bottle eigenstate is to move antiholomorphically under the same eigenmetric of any arbitrary Kaeler-Metric eigenstate. Either way, when one considers a Wilson Line that measures the general length of a sub-mini-string segment, the length of that segment is always 16 times as long as its thickness at its center. Sub-Mini-String is always the same thickness. Again, this is not a length that is derived by a theoretical Gliossi-based Laplacian measurement, yet, this considered length, which is always the same, is based on a Wilson Line that measures the general length of any given sub-mini-string segment. Here is what I mean. Take both ends of any of such said segment. Consider pseudo-orientafolds that extend "above" or "below" a given segment that we are discussing. Draw a line that is straight that connects the orientafolds. That given line will always be the same length, whether the said segment is homeomorphically cylindrical, conically angled at one end, trivially isomrphically conically angled at both ends, or non-trivially isomorphically conically angled at both ends. This is what I mean by a Wilson Line. The ends of sub-mini-string always flushly touch in a Gliossi Manner, whether the given ends are conically angled or not. This goes to show that the slanting of the conically angling of the ends of such said sub-mini-string segments are always bimorphologically isomorphic to the degree that such segments are angled. The number of variations of such slantings is the following: Take the reciprocal of
(~1.104735878*10^(-81)), and divide this number by 16. During the space-hole, the relatively forward holomorphic ends of the segments of sub-mini-string that bind those loci of mini-string (reverse-fractaled of sub-mini-string) that are to temporarily disconnect to retie before the quaternionic-instanton-field-impulse-mode. Such a sub-metric of brief disconnection is due to the virtual lack of a fractal of pressurized vacuum in loci of substringular field. Based on the Laplacian condition that is in consideration of the placement of the substringular field eigenstates as this is happening, the sub-mini-string segment ends that nearly break homotopy reconnect in the manner that involves the least resistance. This retying is what allows for the continuation of Gaussian Transformations, of which allows for the spontaneous kinematic covariance that is essential for metric-gauge to be activated so that superstrings may be discrete energy so that reality may continue. I will continue with the suspence later.
Sub-Mini-String segments bind via an extreme fractal example of a pressurized vacuum. Ideally, one would think that sub-mini-string segments would be flushly homeomorphically cylindrical. Yet, the ends of the segments of sub-mini-string are not necessarily a fractal of cross-sectional orientafolds. Often, either end and/or both ends of sub-mini-string segments are conically angled by up to 11.25 conical degrees if one were to observe such a conical angling at such a close range that a given arbitrary sub-mini-string segment would here appear to be three-dimensional. Such an angling may be singularized, trivially isomorphic when one considers both ends of such a mentionable segment, or non-trivially isomorphic when one considers both ends of such a mentionable segment. So, when such a said segment is non-trivially isomorphic at its maximum conical slanting at both ends, the overall conical angling difference would, in under a Laplacian condition, be a 22.5 degree difference. This coincides with the condition that a Higgs Action eigenstate subtends to an angling of 22.5 degrees to the relative left of a relatively straight up and down subtending when a Klein Bottle eigenstate is to move holomorphically and that the same arbitrary Higgs Action eigenstate subtends to an angling of 22.5 degrees to the relative right from a relatively straight up and down subtending when the respective Klein Bottle eigenstate is to move antiholomorphically under the same eigenmetric of any arbitrary Kaeler-Metric eigenstate. Either way, when one considers a Wilson Line that measures the general length of a sub-mini-string segment, the length of that segment is always 16 times as long as its thickness at its center. Sub-Mini-String is always the same thickness. Again, this is not a length that is derived by a theoretical Gliossi-based Laplacian measurement, yet, this considered length, which is always the same, is based on a Wilson Line that measures the general length of any given sub-mini-string segment. Here is what I mean. Take both ends of any of such said segment. Consider pseudo-orientafolds that extend "above" or "below" a given segment that we are discussing. Draw a line that is straight that connects the orientafolds. That given line will always be the same length, whether the said segment is homeomorphically cylindrical, conically angled at one end, trivially isomrphically conically angled at both ends, or non-trivially isomorphically conically angled at both ends. This is what I mean by a Wilson Line. The ends of sub-mini-string always flushly touch in a Gliossi Manner, whether the given ends are conically angled or not. This goes to show that the slanting of the conically angling of the ends of such said sub-mini-string segments are always bimorphologically isomorphic to the degree that such segments are angled. The number of variations of such slantings is the following: Take the reciprocal of
(~1.104735878*10^(-81)), and divide this number by 16. During the space-hole, the relatively forward holomorphic ends of the segments of sub-mini-string that bind those loci of mini-string (reverse-fractaled of sub-mini-string) that are to temporarily disconnect to retie before the quaternionic-instanton-field-impulse-mode. Such a sub-metric of brief disconnection is due to the virtual lack of a fractal of pressurized vacuum in loci of substringular field. Based on the Laplacian condition that is in consideration of the placement of the substringular field eigenstates as this is happening, the sub-mini-string segment ends that nearly break homotopy reconnect in the manner that involves the least resistance. This retying is what allows for the continuation of Gaussian Transformations, of which allows for the spontaneous kinematic covariance that is essential for metric-gauge to be activated so that superstrings may be discrete energy so that reality may continue. I will continue with the suspence later.
Monday, December 12, 2011
About Point Particles
First-Ordered-Point-Particles comprise superstrings.
Second-Ordered-Point-Particles comprise the mini-string that "balls-up" to form first-ordered-point-particles, while these second-ordered particles also form all mini-string that forms substringular fields.
Third-Ordered-Point-Particles only exist so as to form the composition of second-ordered-point-particles.
Sub-Mini-String binds together third-ordered-point-particles as well as interconnecting the said second-ordered-point-particles.
Just as mini-string forms all substringular fields -- and also considering the condition that second-ordered-point-particles are two orders lower in diameter than superstrings -- sub-mini-string is what binds the mentioned second-ordered-point-particles.
Catch You Two,
Samuel David Roach.
Second-Ordered-Point-Particles comprise the mini-string that "balls-up" to form first-ordered-point-particles, while these second-ordered particles also form all mini-string that forms substringular fields.
Third-Ordered-Point-Particles only exist so as to form the composition of second-ordered-point-particles.
Sub-Mini-String binds together third-ordered-point-particles as well as interconnecting the said second-ordered-point-particles.
Just as mini-string forms all substringular fields -- and also considering the condition that second-ordered-point-particles are two orders lower in diameter than superstrings -- sub-mini-string is what binds the mentioned second-ordered-point-particles.
Catch You Two,
Samuel David Roach.
Wednesday, March 30, 2011
About the Importance of Point Particles to String Theory
In order for superstrings to be able to differentiate and interchange kinematically, there must be point particles that are smaller than these discussed superstrings. A superstring has a length, for 1-D strings, and a circumference, for 2-D strings, of 3*10^(-35) meters in the globally distinguishable. When in a totally contracted state, such a scalar is 10^(-43) meters. A first-ordered-point-particle has a diameter of 10^(-86) meters in the substringular when including the Gliossi Field that is directly associated and thus comprises the said point particle. First-Ordered-Point-Particles are comprised of the substance of the field of superstrings, or, in other words, mini-strings. Mini-String is comprised of second-ordered-point-particles that exist adjacent to each other in exterialy bound "chains" of phenomena that are interconnected by third-ordered-point particles that are bound by sub-mini-string. Second-Ordered-Point-Particles are 10^(-129) meters in diameter in the substringular, third-ordered-point-particles are 10^(-384) meters in diameter in the substringular, and sub-mini-string is 10^(-1152) meters in diameter in the substringular. Sub-Mini-String is the smallest phenomena that is a thing while yet also a gauge-action. Third-Ordered-Point-Particles only exist where there are second-ordered-point-particles. Not only does sub-mini-string bind third-ordered-point-particles together, yet these also work to interconnect the second-ordered-point-particles that comprise mini-string. A physical entity that is smaller than a superstring is termed to be a gauge-action. So how does such a tying of fabric rety while yet maintaining homotopy? The "space-hole" is what I call the duration right before Instanton-Quaternionic-Impulse-Mode, which is right before instanton, which is when homotopy just begins to undue to allow any essential retying of string, yet, to such a minor amount that homotopy during successive instantons is maintained except for when it is frayed in a black-hole. Such a resewing of substringular phenomena is brought back into a multiplicitly discrete homotopy due to the pressure that is impelled upon adjacent superstrings due to the equal and opposite wave-tug of point-particles that acts Gliossi upon the said superstrings to just enough of an extent so as to snap the temporarily untying topology described back into a unified multiplicit homotopic topology.
Wednesday, August 4, 2010
Why Point Particles Are Essential To Motion
Superstrings are made up of first-ordered-point-particles that interconnect via mini-string.
Mini-String comprises first-ordered-point-particles too.
Mini-String is never completely compactified.
Mini-String is composed of second-ordered-point-particles.
Second-Ordered-Point-Particles are composed of third-ordered-point-particles that are composed of sub-mini-string.
Third-Ordered-Point-Particles are connected by sub-mini-string.
Sub-Mini-String is never fully compactified.
Only where there are second-ordered-point-particles are there third-ordered-point-particles.
The kernels of third-ordered-point-particles are interconnected via sub-mini-string.
All unfrayed substringular phenomena is interconnected via sub-mini-string.
Frayed substringular phenomena is patched so that not all phenomena are then frayed, due to Cassimer Invariance.
Cassimer Invariance happens indirectly due to the twisting motion of Fadeev-Popov-Traces during instanton.
Such twisting motion reconnects substringular phenomena in-between instantons to allow for unfrayed space-time-fabric once the first black-holes were formed.
Such an ability from the said twisting is due to the spin-orbital and angular momentum "Gliossi" fields exhibited by third-ordered-point-particles, particularly during what I call the "space-hole."
This is why homotopy is maintained as well as it is.
The "back-and-forth" sway of superstrings during instanton then causes the light-cone-gauge to launch the interconnected points -- such as superstrings and norm-states -- into Ultimon Flow so that there may be Fourier Transforms over the integration of many instantons.
Thus, relative motion may happen within the framework of covariant time without spontaneous fraying.
Orientable strings obey Noether Flow, while unorientable strings become temporarily tachyonic.
Such stated flow is a description of sequential series of Laplacian Transforms of substringular states over the course of many integrated and covariant eigenstates of substringular instantons over the region of many substringular loci.
Please ask me any questions that you may have appertaining to what I have just wrote, since that is how people learn.
Sincerely,
Sam Roach
Mini-String comprises first-ordered-point-particles too.
Mini-String is never completely compactified.
Mini-String is composed of second-ordered-point-particles.
Second-Ordered-Point-Particles are composed of third-ordered-point-particles that are composed of sub-mini-string.
Third-Ordered-Point-Particles are connected by sub-mini-string.
Sub-Mini-String is never fully compactified.
Only where there are second-ordered-point-particles are there third-ordered-point-particles.
The kernels of third-ordered-point-particles are interconnected via sub-mini-string.
All unfrayed substringular phenomena is interconnected via sub-mini-string.
Frayed substringular phenomena is patched so that not all phenomena are then frayed, due to Cassimer Invariance.
Cassimer Invariance happens indirectly due to the twisting motion of Fadeev-Popov-Traces during instanton.
Such twisting motion reconnects substringular phenomena in-between instantons to allow for unfrayed space-time-fabric once the first black-holes were formed.
Such an ability from the said twisting is due to the spin-orbital and angular momentum "Gliossi" fields exhibited by third-ordered-point-particles, particularly during what I call the "space-hole."
This is why homotopy is maintained as well as it is.
The "back-and-forth" sway of superstrings during instanton then causes the light-cone-gauge to launch the interconnected points -- such as superstrings and norm-states -- into Ultimon Flow so that there may be Fourier Transforms over the integration of many instantons.
Thus, relative motion may happen within the framework of covariant time without spontaneous fraying.
Orientable strings obey Noether Flow, while unorientable strings become temporarily tachyonic.
Such stated flow is a description of sequential series of Laplacian Transforms of substringular states over the course of many integrated and covariant eigenstates of substringular instantons over the region of many substringular loci.
Please ask me any questions that you may have appertaining to what I have just wrote, since that is how people learn.
Sincerely,
Sam Roach
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