Dirac neutrinos and gauged lepton number

We propose the first scotogenic neutrino mass model with gauged lepton number <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mi>U</a:mi> <a:mo stretchy="false">(</a:mo> <a:mn>1</a:mn> <a:msub> <a:mo stretchy="false">)</a:mo> <a:mi>L</a:mi> </a:msub> </a:math> , which is spontaneously broken by three units <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mi mathvariant="normal">Δ</e:mi> <e:mi>L</e:mi> <e:mo>=</e:mo> <e:mn>3</e:mn> </e:math> down to a residual discrete gauge symmetry <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"> <h:msub> <h:mi mathvariant="double-struck">Z</h:mi> <h:mn>6</h:mn> </h:msub> </h:math> . The latter guarantees that neutrinos acquire tiny Dirac masses via a one-loop scotogenic mechanism, simultaneously stabilizing the lightest electrically neutral particle with nontrivial charge under the preserved <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"> <k:msub> <k:mi mathvariant="double-struck">Z</k:mi> <k:mn>6</k:mn> </k:msub> </k:math> symmetry. In our model there is a scalar particle identified as weakly interacting massive particle dark matter (DM) candidate. We analyzed its compatibility with the existing data on direct DM detection experiments and the DM relic abundance. We also address charged lepton flavor violating decays in our model and find that their predicted rates are within the reach of current experimental sensitivity.