Distinguishing inert Higgs doublet and inert triplet scenarios
In this article we consider a comparative study between Type-I 2HDM and Y = 0 , SU (2) triplet extensions having one Z 2 -odd doublet and triplet that render the desired dark matter(DM). For the inert doublet model (IDM) either a neutral scalar or pseudoscalar can be the DM, whereas for inert triple...
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Veröffentlicht in: | The European physical journal. C, Particles and fields Particles and fields, 2020-08, Vol.80 (8), p.1-31, Article 715 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | In this article we consider a comparative study between Type-I 2HDM and
Y
=
0
,
SU
(2) triplet extensions having one
Z
2
-odd doublet and triplet that render the desired dark matter(DM). For the inert doublet model (IDM) either a neutral scalar or pseudoscalar can be the DM, whereas for inert triplet model (ITM) it is a CP-even scalar. The bounds from perturbativity and vacuum stability are studied for both the scenarios by calculating the two-loop beta functions. While the quartic couplings are restricted to
0.1
-
0.2
for a Planck scale perturbativity for IDM, these are much relaxed (0.8 ) for ITM. The RG-improved potentials by Coleman-Weinberg show the regions of stability, meta-stability and instability of the electroweak vacuum. The constraints coming from DM relic, the direct and indirect experiments like XENON1T, LUX and H.E.S.S., Fermi-LAT allow the DM mass
≳
700
,
1176
GeV for IDM, ITM respectively. Though mass-splitting among
Z
2
-odd particles in IDM is a possibility for ITM we have to rely on loop-corrections. The phenomenological signatures at the LHC show that the mono-lepton plus missing energy with prompt and displaced decays in the case of IDM and ITM can distinguish such scenarios at the LHC along with other complementary modes. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-020-8271-5 |