Showing posts with label Clifford differentiation. Show all posts
Showing posts with label Clifford differentiation. Show all posts

Monday, April 9, 2018

Solutions To First Three Test Questions Of Test 2 Of Course 20

1)  A Calabi-Yau interaction, is the general interaction that is to happen between the holonomic substrate of discrete quanta of electromagnetic energy -- with the holonomic substrate of orbifold eigensets of mass-bearing discrete quanta of energy.

2)  A tense of a euclidean Clifford differentiation that is involved with electromagnetic energy, is the multiplicit Ward-Cauchy-based condition of the Polyakov Action -- that is relatively minimized for superstrings of mass that bear a velocity that is close to light speed, and is as well being relatively maximized for superstrings of mass that are superconformally invariant in such a manner that is proximal local to a set said region.

3)  In terms of electromagnetic energy, -- the relationship that is to exist between one correlative Polyakov Action eigenstate and its respective Lorentz-Four-Contraction, -- is an example of a Dirac Clifford differentiation.

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

Wednesday, April 4, 2018

Course 20, Session 11, Test 2 Questions

1)  What is a Calabi-Yau interaction?

2)  In terms of electromagnetic energy, what is a euclidean Clifford differentiation?

3)  In terms of electromagnetic energy, what is a Dirac Clifford differentiation?

4)  Explain the Yang-Mills characteristics of electromagnetic energy.

5)  Explain the Kaluza-Klein characteristics of scattered electromagnetic energy.

6)  Explain a typical quantized set of beams of electromagnetic energy.

7)  Explain the orthogonal tense of the light-cone-gauge conditions, that are of scattered electromagnetic energy.

8)  Explain, in terms of both the light-cone-gauge and BRST -- the process that it takes for the re-quantization of electromagnetic energy.

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

Wednesday, September 23, 2009

Addendum 1 to GUFT

The Klein Bottle has an exterior surface area of 768 Planck lengths by 384 Planck lengths. The Klein bottle allows for a group metric of 191 iterations that produce 191 mini-loops to be acquired by each superstring that undergoes the Fourier translation of the set of Kaeler metrics that allows superstrings to attain the permittivity that thee need and to allow their respective Fadeev-Popov-Traces, or, in other words, their Planck phenomenon related phenomena, to attain the impedance that these need to be the discrete units of energy that these are. 768*38*191 = 56,328,192. So, in general, each time that a superstring undergoes 56,328,192 iterations along the ultion whether tachyonic or not since either way these go thru the ultimon or go around the Overall Physical Portion of the space-time-continuum per iteration, the associated discrete units of energy, 56,328,192 iterations after their respective Kaeler metrics, go thru the Klein metric again. The kinematic redifferentiation of superstrings via their Lagrangians through their respective Fourier Transformations allow for redistribution of correlative superstrings and their respective Fadeev-Popov-Traces to allow Minkowski-Wise indistinguishablly different stringular groups that are Hilbert-Wise and Njenhuis-Wise indistinguishablly different stringular groups, seeing that group Ward substringular groups alter in group angle codifferentiation during each successie set of superconformal transposition. When Minkowski-Wise kinematism becomes multiplicit, then the stringular groups associated with the altering Kaeler metrics then become distinguishablly different. This happens when Clifford differentiation becomes Real Reimmanian relative to the associated substrigular fields.