Abstract

Motivated by the long-lasting 3.5σ discrepancy in the anomalous magnetic moment of muon, we consider a new muon-specific force mediated by a light gauge boson, X, with mass mX < 2mμ and the coupling constant gX ∼ (10−4, 10−3) . We show that the Belle II experiment has a robust chance to probe such a light boson in e+e− → μ+μ− + X channel and cover the most interesting parameter space explaining the discrepancy with the planned target luminosity, int dt mathcal{L}=50 {mathrm{ab}}^{-1} . The clean signal of muon-pair plus missing energy at Belle II can be a smoking gun for the new gauge boson. We expect that the (invisibly decaying) muon-philic light (mX ≲ 2mμ) gauge boson can be probed down to gX ≲ 1.5 × 10−4(4.6 × 10−4, 2.3 × 10−4) for 50 (1, 10) ab−1 search.

Highlights

  • Expected sensitivity at Belle IIThe muon-philic gauge bosons are exclusively produced in muon-associated channels is less constrained compared with the model with universal couplings to fermions

  • When we target to the new light gauge boson, Xμ, we don’t really need a huge centerof-mass frame energy of the LHC or other future experiments but rather a precise measurement at a relatively low energy experiment

  • To be specific for muonic force, we have considered the X-bremsstrahlung process e−e+ → μ−μ+X, X → in the muon pair production, which is independent on the kinetic mixing γX

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Summary

Expected sensitivity at Belle II

The muon-philic gauge bosons are exclusively produced in muon-associated channels is less constrained compared with the model with universal couplings to fermions. Belle II experiment, muons are pair-produced and X boson can be radiated away from muon as in figure 3. The signal process is a muon-pair production with the real emission of a light X boson as a final state radiation. This width is very small (ΓX→νν ∼ gX2 mX /12π mX ) in the region of our interests (gX

SM backgrounds and kinematic cuts
Event analysis
Sensitivity limit
Conclusion
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