Abstract

We study the production of a light gauge boson in K−→π−XK^- \to π^- X decay, where the associated new charge current is not conserved. It is found that the process can be generated by the tree-level WW-boson annihilation and loop-induced s→dXs\to dX. We find that it strongly depends on the SU(3)SU(3) limit or the unique gauge coupling to the quarks, whether the decay amplitude of K−→π−XK^-\to π^- X in the WW-boson annihilation is suppressed by mX2εX⋅pKm^2_X ε_X \cdot p_K; however, no such suppression is found via the loop-induced s→dXs\to d X. The constraints on the relevant couplings are studied.

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