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  • Open Access

Bounded from below conditions on a class of symmetry constrained 3HDM

Rafael Boto, Jorge C. Romão, and João P. Silva
Phys. Rev. D 106, 115010 – Published 13 December 2022

Abstract

We study the bounded from below (BFB) conditions on a class of three Higgs doublet models (3HDM) constrained by the symmetry groups U(1)×U(1), U(1)×Z2, and Z2×Z2. These constraints must be implemented on both the neutral (BFB-n) and charged (BFB-c) directions. The exact necessary and sufficient BFB conditions are unknown in the Z2×Z2 case. We develop a general strategy using lower bounds to find sufficient conditions for BFB-n and BFB-c and apply it to these symmetries. In addition, we investigate the concern that the use of safe sufficient conditions can ignore valid points which would yield distinct physical consequences. This is done by performing a full phenomenological simulation of the U(1)×U(1) and U(1)×Z2 models, where exact necessary and sufficient BFB conditions are possible. We look specifically at the points allowed by exact solutions but precluded by safe lower bounds. We found no evidence of remarkable new effects, partly reassuring the use of the lower bounds we propose here, for those potentials where no exact necessary and sufficient BFB conditions are known.

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  • Received 19 August 2022
  • Accepted 14 November 2022

DOI:https://doi.org/10.1103/PhysRevD.106.115010

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

Authors & Affiliations

Rafael Boto*, Jorge C. Romão, and João P. Silva

  • Departamento de Física and CFTP, Instituto Superior Técnico, Universidade de Lisboa, Avenida Rovisco Pais 1, 1049-001 Lisboa, Portugal

  • *rafael.boto@tecnico.ulisboa.pt
  • jorge.romao@tecnico.ulisboa.pt
  • jpsilva@cftp.ist.utl.pt

Article Text

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Issue

Vol. 106, Iss. 11 — 1 December 2022

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Images

  • Figure 1
    Figure 1

    U(1)×U(1): (mA1,mH1±) for Type 1 with the tight Al-2 conditions (left panel) and loose Al-1 conditions (right panel). BFB1=red, BFB2=green, BFB3=orange, BFB4=blue, BFB3+4=gray.

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  • Figure 2
    Figure 2

    Left panel: U(1)×U(1): (λ4,λ7) for Type 1 with the Al-2 conditions. Right panel: U(1)×Z2: (λ4,λ7) for Type 1 with the Al-2 conditions.

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  • Figure 3
    Figure 3

    Z2×Z2: (λ4,λ7) for Type 1 with the Al-2 conditions.

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  • Figure 4
    Figure 4

    Left panel: U(1)×U(1): μZZμγγ plane for the gluon fusion production channel. For Type 1 with Al-2 conditions. Right panel: U(1)×Z2: μZZμγγ plane for the gluon fusion production channel. For Type 1 with Al-2 conditions.

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  • Figure 5
    Figure 5

    Z2×Z2: μZZμγγ plane for the gluon fusion production channel. For Type 1 with Al-2 conditions.

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  • Figure 6
    Figure 6

    Left panel: U(1)×U(1): charged scalar masses for Type 1 with Al-2 conditions. Right panel: U(1)×Z2: charged scalar masses for Type 1 with Al-2 conditions.

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  • Figure 7
    Figure 7

    Z2×Z2: charged scalar masses for Type 1 with Al-2 conditions.

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  • Figure 8
    Figure 8

    Left panel: mH1 versus mA1 for the four sets indicated in the text. Right panel: Same for mH1+ versus mH1+.

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  • Figure 9
    Figure 9

    Left panel: μγγ versus μZZ for the four sets indicated in the text. Right panel: Same for λhhh/λhhhSM versus sin(α1β1).

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