Tuesday, July 23, 2013

A Little Bit Of A Further Description Of The Higgs Boson

When a Higgs Boson eigenstate initially moves a Klein Bottle eigenstate in the relatively norm-to-forward-holomorphic direction, in order for the said Klein Bottle eigenstate to be able to be at the more specific general locus where the directly corresponding Kaeler-Metric eigenstate is to happen -- in so that a Gaussian Transformation may occur at the just mentioned locus, the said Higgs Boson eigenstate pushes the said Klein Bottle eigenstate, via the Fischler-Suskind-Mechanism -- with its "tip" being pulled flushly in the same specific direction that the center of the norm-to-forward-holomorphic end of the mentioned Klein Bottle eigenstate is moving, over the course of that motion in which the stated Higgs Boson eigenstate works to move the eluded to Schotky Construction toward the described locus where superstrings that are of the same substringular neighborhood that are of discrete energy permittivity are to enter the just mentioned Construction so that these said superstrings may re-attain the discrete permittivity indices that these said superstrings need in order that these strings may remain as fundamental discrete units of energy permittivity -- so that energy may exist at all.  At the same general metrical condition of duration that superstrings work to re-attain being discrete units of energy permttivity, their directly corresponding Fadeev-Popov-Ghosts enter the Schotky Construction in order to re-attain discrete energy impedance.  As the stated given arbitrary Klein Bottle eigenstate is reiterated in a kinematic pull per group instanton in the relative forward holomorphic direction, the directly related Higgs Boson eigenstate is angled at 22.5 degrees counterclockwise From a flush pull in the relative norm-to-holomorphic direction at the locus of the Poincaire of the said tip of the stated Higgs Boson eigenstate  -- this, of which would be 67.5 degrees subtended from angling in the direct relative forward-holomorphic direction, when again, is at the locus of the Poincaire of the said tip of the stated Higgs Boson eigenstate.  When the Klein Bottle eigenstate of this given arbitrary example is then to move in the relative reverse-holomorphic direction over the course of the Kaeler-Metric, then, the stated tip of the Higgs Action eigenstate that is here being discussed is pulled 45 degrees clockwise in so as to then be subtended at 22.5 degrees in the opposite direction From a flush pull in the relative forward-norm-to-holomorphic direction. So as the Schotky Construction is to move in the relative reverse-norm-to-holomorphic direction, then, the directly related Higgs Boson eigenstate is angled flushly in the center of the direction in which the correlative Klein Bottle eigenstate is to move in over this part of the activity of the Fischler-Suskind-Mechanism, in which the stated Klein Bottle eigenstate is to here now move, at least temporarily, out of the specific locus of the activity of the Kaeler-Metric. In each case, Higgs Action eigenstates always are Gliossi at the general Poincaire of the relatively reverse-norm-to-holomorphic positioning of the holonomic substrate of their corresponding Klein Bottle eigenstates.  I will continue with the suspense later.  P.S.:  Even thought my wording may not be perfect, the picture in my mind as to this is as clear as can be!  Sincerely, Sam Roach.

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