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Reappraisal of the wrong-sign hbb¯ coupling and the study of hZγ

Duarte Fontes, J. C. Romão, and João P. Silva
Phys. Rev. D 90, 015021 – Published 18 July 2014

Abstract

It has been pointed out recently that current experiments still allow for a two Higgs doublet model where the hbb¯ coupling (kDmb/v) is negative; a sign opposite to that of the Standard Model. Due to the importance of delayed decoupling in the hH+H coupling, hγγ improved measurements will have a strong impact on this issue. For the same reason, measurements or even bounds on hZγ are potentially interesting. In this article, we revisit this problem, highlighting the crucial importance of hVV, which can be understood with simple arguments. We show that the impacts on kD<0 models of both hbb¯ and hτ+τ are very sensitive to input values for the gluon fusion production mechanism; in contrast, hγγ and hZγ are not. We also inquire if the search for hZγ and its interplay with hγγ will impact the sign of the hbb¯ coupling. Finally, we study these issues in the context of the flipped two Higgs doublet model.

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  • Received 2 July 2014

DOI:https://doi.org/10.1103/PhysRevD.90.015021

© 2014 American Physical Society

Authors & Affiliations

Duarte Fontes1,*, J. C. Romão1,†, and João P. Silva2,1,‡

  • 1Centro de Física Teórica de Partículas (CFTP), Instituto Superior Técnico, Universidade de Lisboa, 1049-001 Lisboa, Portugal
  • 2Instituto Superior de Engenharia de Lisboa-ISEL, 1959-007 Lisboa, Portugal

  • *duartefontes@tecnico.ulisboa.pt
  • jorge.romao@tecnico.ulisboa.pt
  • jpsilva@cftp.tecnico.ulisboa.pt

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Vol. 90, Iss. 1 — 1 July 2014

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Images

  • Figure 1
    Figure 1

    Left panel: Assuming that all μf are within 20% of the SM prediction we plot μbb¯ (red/dark gray) and μγγ (black). Right panel: Assuming now that μVV are within 5% of the SM prediction we plot the same quantities. For comparison we also plot μbb¯ (cyan/light gray) for the assumed production of Ref. [7].

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  • Figure 2
    Figure 2

    Left panel: Plot of tanβ as a function of sinα for all the points that obey Eq. (10) with 0.8μVV1.2. Right panel: Plot of sin2(βα) as a function of tanβ for the points that obey Eq. (10) with 0.8μVV1.2 and have kD<0.

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  • Figure 3
    Figure 3

    Fractional variation of sin2(βα) as a function of tanβ for all points with kD<0 that obey Eq. (10) with 0.8μVV1.2.

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  • Figure 4
    Figure 4

    Left panel: kD2 as a function of sin2(βα) for all points with kD<0 that obey Eq. (10) with 0.8μVV1.2 (black) or with 0.95μVV1.05 (cyan/light gray). Right panel: The same but for generated data obeying the model constraints.

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  • Figure 5
    Figure 5

    Allowed region for kD2 as a function of sin2(βα) for all points with kD<0 that obey 0.8μVV1.2 (black). The region in cyan (light gray) is obtained by imposing in addition that 0.8μττ1.2, while in the region in red (dark gray) we further impose 0.8μγγ1.2.

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  • Figure 6
    Figure 6

    Same as in Fig. 5, but for the assumed production rates in Ref. [7]. See text for details.

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  • Figure 7
    Figure 7

    Left panel: Prediction for μτ+τ (red/dark gray) and μγγ (black) as a function of tanβ for the LHC at 14 TeV with the constraint of 20% errors at 8 TeV. Right panel: Assuming now that μVV are within 5% of the SM prediction at 14 TeV, we plot the same quantities. Also shown (cyan/light gray) is the prediction for μbb¯(Vh) from associated production.

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  • Figure 8
    Figure 8

    Prediction for μτ+τ (red/dark gray), μZγ (cyan/light gray), and μγγ (black) as a function of tanβ, for the LHC at 14 TeV, with a measurement of μVV within 5% of the SM at 14 TeV.

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  • Figure 9
    Figure 9

    Predictions for μZγ versus μγγ at 14 TeV, for kD<0. In black, we have the points in the SET (obeying theoretical constraints and S,T,U, only). In red/dark gray (cyan/light gray), the points satisfying, in addition, VV within 20% (5%) of the SM, at 14 TeV.

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  • Figure 10
    Figure 10

    Predictions for μZγ versus μγγ at 14 TeV, for kD>0. In black, we have the points in the SET (obeying theoretical constraints and S,T,U, only). In red/dark-gray (cyan/light gray), the points satisfying, in addition, VV within 20% (5%) of the SM, at 14 TeV.

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  • Figure 11
    Figure 11

    Left panel: Allowed region for kD2 as a function of sin2(βα) in the flipped 2HDM, for all points with kD<0 that obey 0.8μVV1.2 (black). The region in cyan (light gray) is obtained by imposing, in addition, that 0.8μττ1.2, while in the region in red (dark gray) we further impose 0.8μγγ1.2. Right panel: Predictions for μZγ versus μγγ at 14 TeV, for kD<0, in the flipped 2HDM. In black, we have the points in the SET (obeying theoretical constraints and S,T,U, only). In red/dark gray (cyan/light gray), the points satisfying, in addition, VV within 20% (5%) of the SM, at 14 TeV. Shown in green/light gray are the points satisfying μτ+τ at 20% of the SM, which lie on a line going diagonally from the origin with almost unit slope.

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