2015
DOI: 10.1007/jhep05(2015)128
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Two-loop contributions of the order O α t α s $$ \mathcal{O}\left({\alpha}_t{\alpha}_s\right) $$ to the masses of the Higgs bosons in the CP-violating NMSSM

Abstract: Abstract:We provide the two-loop corrections to the Higgs boson masses of the CPviolating NMSSM in the Feynman diagrammatic approach with vanishing external momentum at O(α t α s ). The adopted renormalization scheme is a mixture between DR and on-shell conditions. Additionally, the renormalization of the top/stop sector is provided both for the DR and the on-shell scheme. The calculation is performed in the gaugeless limit. We find that the two-loop corrections compared to the one-loop corrections are of the … Show more

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Cited by 43 publications
(81 citation statements)
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References 133 publications
(154 reference statements)
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“…In these two cases, CP-violation enters the Higgs sector via radiative corrections, JHEP06(2015)052 where the leading effect is generated by the sfermion corrections. On the other hand, the mass obtained with our code is independent from φ M 3 , while such a dependence already appears at one-loop in [89]. Note that one does not expect gluino corrections to the Higgs mass at one-loop order and it is thus not surprising that our implementation does not show JHEP06(2015)052 any variation with φ M 3 .…”
Section: Jhep06(2015)052mentioning
confidence: 64%
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“…In these two cases, CP-violation enters the Higgs sector via radiative corrections, JHEP06(2015)052 where the leading effect is generated by the sfermion corrections. On the other hand, the mass obtained with our code is independent from φ M 3 , while such a dependence already appears at one-loop in [89]. Note that one does not expect gluino corrections to the Higgs mass at one-loop order and it is thus not surprising that our implementation does not show JHEP06(2015)052 any variation with φ M 3 .…”
Section: Jhep06(2015)052mentioning
confidence: 64%
“…If we blindly input the parameters given in section 4.1 of this reference into our framework, 9 the spectrum -not unexpectedly and already with the CP-conserving NMSSSMTools -turns out to be slightly different from the quoted one: in particular, the mostly CP-even and mostly CP-odd singlet states appear with masses ∼ 108 GeV and ∼ 113 GeV respectively. Yet, this discrepancy can be absorbed within a small shift of A κ cos ϕ 2 : using the value 203 GeV, we then recover states at ∼ 103 and ∼ 128 GeV so that the Higgs spectrum then largely coincides with the one provided in [89].…”
Section: Jhep06(2015)052mentioning
confidence: 76%
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