Emergent new symmetry from the Higgs shadow

We show in this Letter how a new hidden gauge symmetry responsible for neutrino mass as well as dark matter (DM) in the Universe can be discovered through scalar mediators responsible for breaking the new symmetry. The new force mediator ( Z (cid:48) ) may be lighter than the Standard Model (SM) gauge bosons but cannot be observed in traditional searches for new gauge bosons. We highlight a novel way of discovering such a symmetry at the Large Hadron Collider (LHC) by incorporating an existing ATLAS analysis on four lepton final states which include the Higgs resonance. In addition, we show that the hidden sector also introduces flavor violation in the lepton sector which can become a significant channel of discovery for the new force.

[1]  X. Marcano,et al.  Z lepton flavour violation as a probe for new physics at future e+e-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$e^ , 2021, The European Physical Journal C.

[2]  A. Sopczak Precision Measurements in the Higgs Sector at ATLAS and CMS , 2020, 2001.05927.

[3]  R. B. Barreiro,et al.  Planck 2018 results , 2018, Astronomy & Astrophysics.

[4]  Arnulf Quadt,et al.  Oxford University Press : Review of Particle Physics, 2020-2021 , 2020 .

[5]  J. T. Childers,et al.  FCC-ee: The Lepton Collider , 2019, The European Physical Journal Special Topics.

[6]  Atlas Collaboration Search for invisible Higgs boson decays in vector boson fusion at $\sqrt{s} = 13$ TeV with the ATLAS detector , 2018, 1809.06682.

[7]  X. Marcano,et al.  One-loop effective LFV $$\varvec{Zl_kl_m}$$Zlklm vertex from heavy neutrinos within the mass insertion approximation , 2018, The European Physical Journal C.

[8]  S. Rai,et al.  New signals for vector-like down-type quark in U(1) of E6\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$E_6$$\end{doc , 2017, The European Physical Journal C.

[9]  L. A. Antonelli,et al.  Limits to dark matter annihilation cross-section from a combined analysis of MAGIC and Fermi-LAT observations of dwarf satellite galaxies , 2016, 1601.06590.

[10]  Hiren H. Patel Package-X: A Mathematica package for the analytic calculation of one-loop integrals , 2015, Comput. Phys. Commun..

[11]  Peter Skands,et al.  An introduction to PYTHIA 8.2 , 2014, Comput. Phys. Commun..

[12]  Jong Soo Kim,et al.  CheckMATE: Confronting your favourite new physics model with LHC data , 2013, Comput. Phys. Commun..

[13]  D. Hooper,et al.  The characterization of the gamma-ray signal from the central Milky Way: A case for annihilating dark matter , 2014, 1402.6703.

[14]  Oscar Stål,et al.  HiggsSignals: Confronting arbitrary Higgs sectors with measurements at the Tevatron and the LHC , 2013, 1305.1933.

[15]  A. Belyaev,et al.  $W'$ and $Z'$ searches at the LHC , 2013 .

[16]  Andy Buckley,et al.  Rivet user manual , 2010, Comput. Phys. Commun..

[17]  The Cms Collaboration Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC , 2012, 1207.7235.

[18]  W. Marsden I and J , 2012 .

[19]  Georg Weiglein,et al.  HiggsBounds 2.0.0: Confronting neutral and charged Higgs sector predictions with exclusion bounds from LEP and the Tevatron , 2011, Comput. Phys. Commun..

[20]  Georg Weiglein,et al.  HiggsBounds: Confronting arbitrary Higgs sectors with exclusion bounds from LEP and the Tevatron , 2008, Comput. Phys. Commun..

[21]  P. Langacker,et al.  Neutralino relic density in a supersymmetric U(1)' model , 2004, hep-ph/0408120.

[22]  E. Ma Neutrino masses in an extended gauge model with E6 particle content , 1995, hep-ph/9507348.

[23]  M. Pérez-Victoria,et al.  Physical parameters and renormalization of U(1)a × U (1)b models , 1995, hep-ph/9507455.