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We examine a generic field theory in which the field particle has twocouplings. It is of particular interest when these are the electroweak, e, andthe hypothetical magnetoweak, g. The new field operators are obtained byreplacing the field operators $\Psi (x)$ of the standard model or of similarmodels by $\tilde{\Psi} (x) D^j_q (m,m')$ where $ D^j_q (m,m')$ is an elementof the $2j+1$ dimensional representation of the SLq(2) algebra, which is alsothe knot algebra. The field is assumed to exist in two phases distinguished bytwo values of $q$: $q_e = \frac{e}{g}$ and $q_g = \frac{g}{e}$ which label theelectroweak and magnetoweak phases respectively.  We assume that the observed leptons and quarks are composed of e-preons andare in agreement with the observed charge spectrum of leptons and quarks. It isnow proposed that there is also a g-phase where g-leptons and g-quarks arecomposed of g-preons. It is assumed that the g-charge is very large compared tothe e-charge and the mass of the g charged particle is even larger since themass of all of these particles is partially determined by the eigenvalues of$\bar{D}^j_q (m,m') D_q^j (m,m')$, a polynomial in $q$, that multiplies theHiggs mass term and where \begin{equation*} \frac{q_g}{q_e} = \left (\frac{\hbar c}{e^2} \right)^2 \approx (137)^2. \end{equation*}  These values of $q$ indicate that particles in the g-phase are much moremassive, they should be harder to produce or to observe.

The Concept of Electric Charge and the Hypothesis of Magnetic Poles