Tuesday, January 25, 2011

Theory Update 39

Now we could use a Fun representation of braids, as discussed in this paper, where the Fourier type transform uses both ordinary matrix multiplication and a permutation transformation $P$ to recover the Z boson diagonal.
This takes a flat neutrino diagram in $B_3$ and creates twists in copies of $B_2$. As we have seen, quarks and charged leptons (in $B_6$ perhaps) are also needed to define the transform.

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