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Weak Nuclear Force

Responsible for certain types of radioactive decay, mediating reactions involving changes in the neutron-to-proton ratio.
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The statement of the theorem

The weak interaction is described by the effective Lagrangian Lweak\mathcal{L}_{weak} involving the exchange of W±W^{\pm} and Z0Z^0 bosons. For a process like beta decay (np+e+νˉen \to p + e^- + \bar{\nu}_e), the interaction Hamiltonian density Hint\mathcal{H}_{int} is derived from the coupling of the leptonic current JLJ_L and the hadronic current JHJ_H: \nHint=GF2JLμJHμ+h.c.\mathcal{H}_{int} = \frac{G_F}{\sqrt{2}} J_L^{\mu} J_{H}^{\mu} + \text{h.c.} \nWhere GFG_F is the Fermi constant, and JLJ_L and JHJ_H are the respective weak currents.