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Phenomenology of CP-even ALP

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arxiv 2111.03653 v2 pith:CKGDGAZL submitted 2021-11-05 hep-ph astro-ph.COhep-ex

classification hep-phastro-ph.COhep-ex
keywords decaycp-evenhiggsbosonparticlecollidersdisplacedlight
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Axion or axion-like particle (ALP) has been usually considered as a CP-odd Nambu-Goldstone boson (NGB) from the spontaneous breakdown of a global U(1) symmetry. In this paper, we point out that the NGB behaves as a CP-even particle coupled to the SM particles in a large class of simple (or perhaps the simplest) renormalizable models. We provide a first study of the collider phenomenology and cosmology of the CP-even ALP. In a natural parameter region, the CP-even ALP can be produced from the Higgs boson decay in colliders. When the mass is not very light, the signals will be Higgs exotic decays, Higgs decay to displaced vertex $\times 2$, Higgs decay to displaced vertex + missing energy. The signal can be discriminated from other models, e.g. hidden photon, by measuring the decay length and the decay products of the light new particle. In addition, when $ m_a\lesssim \,$MeV, in which case the Higgs boson invisible decay may be probed in the colliders, the CP-even ALP is a nice Dark matter (DM) candidate. The DM can be probed by 21cm line measurement, the future measurement of the Milky way mass halo function in the Vera Rubin Observatory, as well as X- or $\gamma$-ray observations. The DM production mechanisms are discussed.

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