Abstract

We explore supersymmetric theories in which the Higgs mass is boosted by the non-decoupling D-terms of an extended $U(1)_X$ gauge symmetry, defined here to be a general linear combination of hypercharge, baryon number, and lepton number. Crucially, the gauge coupling, $g_X$, is bounded from below to accommodate the Higgs mass, while the quarks and leptons are required by gauge invariance to carry non-zero charge under $U(1)_X$. This induces an irreducible rate, $\sigma$BR, for $pp \rightarrow X \rightarrow \ell\ell$ relevant to existing and future resonance searches, and gives rise to higher dimension operators that are stringently constrained by precision electroweak measurements. Combined, these bounds define a maximally allowed region in the space of observables, ($\sigma$BR, $m_X$), outside of which is excluded by naturalness and experimental limits. If natural supersymmetry utilizes non-decoupling D-terms, then the associated $X$ boson can only be observed within this window, providing a model independent `litmus test' for this broad class of scenarios at the LHC. Comparing limits, we find that current LHC results only exclude regions in parameter space which were already disfavored by precision electroweak data.

Highlights

  • Experimental constraintsWe analyze the experimental constraints on general U(1)X extensions of the MSSM

  • Non-trivial limits can be derived without exact knowledge of seemingly essential parameters like gX, p, and q

  • We explore supersymmetric theories in which the Higgs mass is boosted by the non-decoupling D-terms of an extended U(1)X gauge symmetry, defined here to be a general linear combination of hypercharge, baryon number, and lepton number

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Summary

Experimental constraints

We analyze the experimental constraints on general U(1)X extensions of the MSSM. The relevant bounds come from the mass of the Higgs boson, precision electroweak measurements, and direct limits from the LHC. Contributions to precision electroweak observables arise from two sources: mixing between the X and Z bosons, and couplings between the X boson and leptons The former is always generated by electroweak symmetry breaking since the Higgs is, by construction, charged under U(1)X. The latter is always present, since X has an irreducible coupling to leptons. The leptonic branching ratios are given in eq (3.5) as a function of p and q, while the production cross-section of X bosons from proton collisions can be computed in terms of p with MadGraph, including NNLO corrections from [23]. ΣBR is non-zero for any value of p and q, as shown in figure 5, which shows the rate normalized to gX2 for a sample parameter space point, mX

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