<p>The Direct Detection (DD) experiments are vital for probing the particle nature of Dark Matter (DM). However, in the absence of a scattering event, DD searches result in stringent bounds on the corresponding parameter space. The paper has considered a <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="normal">U</mi> <msub> <mfenced close=")" open="("> <mn>1</mn> </mfenced> <mrow> <msub> <mi>L</mi> <mi>μ</mi> </msub> <mo>−</mo> <msub> <mi>L</mi> <mi>τ</mi> </msub> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">\( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \)</EquationSource> </InlineEquation> -extension of the Standard Model (SM) and augmented the particle spectrum with SU(2)<sub><i>L</i></sub>-singlet vector-like leptons and scalars. A discrete <i>Z</i><sub>2</sub> symmetry stabilizes the lightest SM-singlet vector-like lepton as the viable DM candidate. In the proposed model, amplitude-level cancellation can be achieved for both DM-electron and DM-quark scatterings, leading to a trivial explanation for the continuous null results in the DD experiments. The framework can also induce one-loop corrections to the lepton anomalous magnetic moments and <i>Zℓ</i><sup>+</sup><i>ℓ</i><sup>−</sup> couplings. The experimental bounds on the <i>Z</i> → <i>ℓ</i><sup>+</sup><i>ℓ</i><sup>−</sup> decays are instrumental in constraining the model parameters. Particularly, using the <i>Z</i> → <i>τ</i> <sup>+</sup><i>τ</i> <sup>−</sup> decay, a stronger exclusion limit can be imposed on the <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="normal">U</mi> <msub> <mfenced close=")" open="("> <mn>1</mn> </mfenced> <mrow> <msub> <mi>L</mi> <mi>μ</mi> </msub> <mo>−</mo> <msub> <mi>L</mi> <mi>τ</mi> </msub> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">\( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \)</EquationSource> </InlineEquation> parameter space. Further, in the presence of three heavy right-handed neutrinos, transforming as <i>Z</i><sub>2</sub>-even states, the model can explain all the neutrino mass and mixing constraints using the Type-I seesaw mechanism. Future experimental updates on the (<i>g</i> − 2)<sub><i>ℓ</i></sub>, <i>Z</i> → <i>ℓ</i><sup>+</sup><i>ℓ</i><sup>−</sup> decays and improved bounds on the <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="normal">U</mi> <msub> <mfenced close=")" open="("> <mn>1</mn> </mfenced> <mrow> <msub> <mi>L</mi> <mi>μ</mi> </msub> <mo>−</mo> <msub> <mi>L</mi> <mi>τ</mi> </msub> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">\( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \)</EquationSource> </InlineEquation> theory can be crucial to test the proposed model. Moreover, future DD experiments searching for a DM-muon scattering might be significant to probe the considered DM-SM interaction.</p>

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Exploring the null results in the direct detection experiments, (g − 2) and neutrino mass in an extended \( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \) model constrained through the Z+ decays

  • Bibhabasu De

摘要

The Direct Detection (DD) experiments are vital for probing the particle nature of Dark Matter (DM). However, in the absence of a scattering event, DD searches result in stringent bounds on the corresponding parameter space. The paper has considered a U 1 L μ L τ \( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \) -extension of the Standard Model (SM) and augmented the particle spectrum with SU(2)L-singlet vector-like leptons and scalars. A discrete Z2 symmetry stabilizes the lightest SM-singlet vector-like lepton as the viable DM candidate. In the proposed model, amplitude-level cancellation can be achieved for both DM-electron and DM-quark scatterings, leading to a trivial explanation for the continuous null results in the DD experiments. The framework can also induce one-loop corrections to the lepton anomalous magnetic moments and Zℓ+ couplings. The experimental bounds on the Z+ decays are instrumental in constraining the model parameters. Particularly, using the Zτ +τ decay, a stronger exclusion limit can be imposed on the U 1 L μ L τ \( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \) parameter space. Further, in the presence of three heavy right-handed neutrinos, transforming as Z2-even states, the model can explain all the neutrino mass and mixing constraints using the Type-I seesaw mechanism. Future experimental updates on the (g − 2), Z+ decays and improved bounds on the U 1 L μ L τ \( \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} \) theory can be crucial to test the proposed model. Moreover, future DD experiments searching for a DM-muon scattering might be significant to probe the considered DM-SM interaction.