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Patrick Foldenauer

Publications and source records attributed to Patrick Foldenauer.

20 records · Page 2Linked to original sources

Let there be Light Dark Matter: The gauged $U(1)_{L_μ-L_τ}$ case

As experimental null results increase the pressure on heavy weakly interacting massive particles (WIMPs) as an explanation of thermal dark matter (DM), it seems timely to explore previously overlooked regions of the WIMP parameter space. In this work we extend the minimal gauged $U(1)_{L_μ-L_τ}$ model studied in \cite{Bauer:2018onh} by a light (MeV-scale) vector-like fermion $χ$. Taking into account constraints from cosmology, direct and indirect detection we find that the standard benchmark of $M_V=3 m_χ$ for DM coupled to a vector mediator is firmly ruled out for unit DM charges. However, exploring the near-resonance region $M_V\gtrsim 2 m_χ$ we find that this model can simultaneously explain the DM relic abundance $Ωh^2 =0.12$ and the $(g-2)_μ$ anomaly. Allowing for small charge hierarchies of $\lesssim\mathcal{O}(10)$, we identify a second window of parameter space in the few-GeV region, where $χ$ can account for the full DM relic density.

hep-ph↗

Purely flavor-changing Z' bosons and where they might hide

A plethora of ultraviolet completions of the Standard Model have extra U(1) gauge symmetries. In general, the associated massive $Z^\prime$ gauge boson can mediate flavor-changing neutral current processes at tree level. We consider a situation where the $Z^\prime$ boson couples solely via flavor-changing interactions to quarks and leptons. In this scenario the model parameter space is, in general, quite well constrained by existing flavor bounds. However, we argue that cancellation effects shelter islands in parameter space from strong flavor constraints and that these can be probed by multipurpose collider experiments like ATLAS or CMS as well as LHCb in upcoming runs at the LHC. In still allowed regions of parameter space these scenarios may help to explain the current tension between theory and experiment of $(g-2)_μ$ as well as a small anomaly in $τ$ decays.

hep-ph↗