Abstract
We show that new physics explanations of the muon $g-2$ anomaly by the contributions of new leptons mediated by the standard model Higgs boson necessarily lead to large rates for $\mu^+ \mu^- \to hh$ and $\mu^+ \mu^- \to hhh$ irrespectively of details of the model or the scale of new physics. For new leptons with the same quantum numbers as the standard model leptons, cross sections are expected to be about 240 ab for $\mu^+ \mu^- \to hh$ independently of the center of mass energy, $\sqrt{s}$, and about 2.7 ab for $\mu^+ \mu^- \to hhh$ for $\sqrt{s} = 1$ TeV and growing quadratically with $\sqrt{s}$. Predictions for models featuring new leptons with different quantum numbers and for a type-II two Higgs doublet model, where additional Higgs bosons can contribute to muon $g-2$, are also presented.
Highlights
The measured value of the muon anomalous magnetic moment, aμ 1⁄4 ðg − 2Þμ=2, represents one of the most significant deviations from predictions of the standard model (SM)
We show that new physics explanations of the muon g − 2 anomaly by the contributions of new leptons mediated by the standard model Higgs boson necessarily lead to large rates for μþμ− → hh and μþμ− →
It turns out that for new leptons with the same quantum numbers as SM leptons, the one sigma range of ðg − 2Þμ is consistent with the SM prediction for h → μþμ−, and exactly the SM value is predicted for ðg − 2Þμ just slightly below the current central value [4]
Summary
The measured value of the muon anomalous magnetic moment, aμ 1⁄4 ðg − 2Þμ=2, represents one of the most significant deviations from predictions of the standard model (SM). The possible mass enhancement in these contributions allows for very heavy leptons, far beyond the reach of future colliders, and the confirmation of such explanations might solely rely on indirect evidence Such indirect evidence includes modifications of muon couplings to Z, W and Higgs bosons from SM predictions. For new leptons with the same quantum numbers as SM leptons, cross sections are expected to be about 240 ab fopr μffiffiþ masspeffiffinergy, s, μ− → and hh independently of the center of about 2.7 ab for μþμ− → hphffihffi for s 1⁄4 1 TeV and growing quadratically with s This presents a unique discovery opportunity, where the scenario could be tested even at low energies. We discuss related mixed diHiggs and tri-Higgs signals in 2HDM and signals in models with new mediators not participating in electroweak symmetry breaking (EWSB)
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