paper

On the SLq(2) extension of the standard model and the measure of charge

arXiv:1511.07919 · doi:10.1142/S0217751X17300010

Abstract

Our SLq(2) extension of the standard model is constructed by replacing the elementary field operators, , of the standard model by where is an element of the dimensional representation of the SLq(2) algebra, which is also the knot algebra. The allowed quantum states are restricted by the topological conditions \begin{equation*} (j,m,m') = \frac{1}{2}(N,w,r+o) \end{equation*} postulated between the states of the quantum knot and the corresponding classical knot where the are (the number of crossings, the writhe, the rotation) of the 2d projection of the corresponding oriented classical knot. Here is an odd number that is required by the difference in parity between and . There is also the empirical restriction on the allowed states \begin{equation*} (j,m,m')=3(t,-t_3,-t_0)_L \end{equation*} that holds at the level, connecting quantum trefoils with leptons and quarks . The so constructed knotted leptons and quarks turn out to be composed of three particles which unexpectedly agree with the preon models of Harrari and Shupe. The particles, being electroweak neutral, are dark and plausibly greatly outnumber the quarks and leptons. The SLq(2) or measure of charge has a direct physical interpretation since is the total number of preonic charges while and are the numbers of writhe and rotation sources of preonic charge. The total SLq(2) charge of a particle, measured by writhe and rotation and composed of preons, sums the signs of the counterclockwise turns and clockwise turns that any energy-momentum current makes in going once around the knot... Keywords: Quantum group; electroweak; knot models; preon models; dark matter.

21 pages, 3 figures. arXiv admin note: text overlap with arXiv:1401.1833

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