Re: Update on Weinberg-Sallam model in super symmetry as E8xE8-> energy of split

*To*: mathgroup at smc.vnet.net*Subject*: [mg70336] Re: Update on Weinberg-Sallam model in super symmetry as E8xE8-> energy of split*From*: Roger Bagula <rlbagula at sbcglobal.net>*Date*: Fri, 13 Oct 2006 01:30:44 -0400 (EDT)*References*: <egl44b$53a$1@smc.vnet.net>

Roger Bagula wrote: >I spent yesterday learning about super symmetric Higgs symmetry breaking >theory. > > > > > Sorry about the spelling in the title, ha, ha... The bonding model for the "between " super symmetry model that comes to mind is the trigonal prism: A120656 6by6 trigonal prism bonding graph matrix Markov: this molecular structure is the major symmetry between the tetrahedron and cube: characteristic polynomial:12 x^2 - 4 x^3 - 9 x^4 + x^6. The problem with that is it puts the energy for the H+,H- state between the Z0 and W+,W-. {-2,-2,0,0,1,3} An alternative is the octahedral: A120470 6X6 Matrix Markov of the octahedral bonding graph. {-2., -2., 0., 0., 0., 4.} That puts energy of Z0->H+,H- and ? H0=3*MW~273.6 gev Which is much higher than I would expect. My idea was that they would be symmetrical like: {-A,-B,-B,B,B,A} So that MH0=2*MZ0~ 182.3 gev MH(+/-)=2*MW~160.6 gev I have got a 6by6 bonding model that gives that as a cyclic bonding ( like benzene) : {-2., -1., -1., 1., 1., 2.}->{Z0,W+,W-,H+,H-,H0} A120462 6 X 6 Matrix Markov based on hexagon / benzene chemical bonding type Markov with characteristic polynomial : x^6-6*x^4+9*x^2-4. Mathematica: M = {{0, 1, 1, 1, 0, 0}, {1, 0, 1, 0, 1, 0}, {1, 1, 0, 0, 0, 1}, {1, 0, 0, 0, 1, 1}, {0, 1, 0, 1, 0, 1}, {0, 0, 1, 1, 1, 0}} v[1] = {0, 1, 1, 2, 3, 5} v[n_] := v[n] = M.v[n - 1] a = Table[Floor[v[n][[1]]], {n, 1, 50}] Det[M - x*IdentityMatrix[6]] Factor[%] aaa = Table[x /. NSolve[Det[M - x*IdentityMatrix[6]] == 0, x][[ n]], {n, 1, 6}] Abs[aaa] a1 = Table[N[a[[n]]/a[[n - 1]]], {n, 7, 50}] I will not imply mine is better than nature, so each of these possibility is about equally likely.