Summary plots from the ATLAS Higgs physics group
Contact: ATLAS Higgs conveners
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Higgs mass:
Summary of the Higgs boson mass measurements from the individual and combined analyses performed here, compared with the combined Run 1 measurement by ATLAS and CMS [6]. The statistical-only (horizontal yellow-shaded bands) and total (black error bars) uncertainties are indicated. The (red) vertical line and corresponding (grey) shaded column indicate the central value and the total uncertainty of the combined ATLAS Run 1 + 2 measurement, respectively. Reference: Figure 4 in arXiv:1806.00242

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Run 1 Spin/CP:
Distributions of the test statistic q for the SM Higgs boson and for the JP alternative hypotheses. They are obtained by combining the H → ZZ* → 4 ℓ , H → WW* → e ν μ ν and H → γ γ decay channels. The expected median (black dashed line) and the ±1, ±2 and ±3 σ regions for the SM Higgs boson (blue) and for the alternative JP hypotheses (red) are shown for the signal strength fitted to data. The observed q values are indicated by the black points. Reference: Auxiliary Figure 5 in Eur. Phys. J. C75 (2015) 476

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Total pp → H + X cross section as function of sqrt(s) from H→ γ γ and H→ ZZ* → 4ℓ:
Total pp → H + X cross sections measured at centre-of-mass energies of 7, 8, and 13 TeV, compared to Standard Model predictions at up to N3LO in QCD. Shown are the measurements in the H→ γ γ channel (red triangles), the H→ ZZ* → 4ℓ channel (green rectangles), and the combinations of these two channels (black dots). The individual channel results are offset along the x-axis for display purposes. The grey bands on the combined measurements represent the systematic uncertainty, while the error bars show the total uncertainty. The light (dark) blue band shows the estimated uncertainty due to missing higher-order corrections (the total uncertainty). The total theoretical uncertainty corresponds to the higher-order-correction uncertainty summed in quadrature with the sum of the PDF and αS uncertainties, and is partially correlated across values of the centre-of-mass energy. Reference: Figure 1 in ATLAS-CONF-2017-047

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Run 1 cross section and partial decay width ratios:
The gg→ H→ WW* cross section, ratios of cross sections and of partial decay widths relative to their SM values at mH=125.36 GeV from the combined analyses of the √s=7 and 8 TeV data. The inner and outer error bars on the measurements are 68% CL and 95% CL intervals. The SM predictions are shown as the vertical line at unity with grey bands representing theoretical uncertainties on the ratios of inclusive cross sections and of partial decay widths. Reference: Figure 6 in Eur. Phys. J. C (2016) 76:6

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Run 2 cross section and partial decay width ratios:
Results of a simultaneous fit for σggFZZ, σVBFggF, σWHggF, σZHggF, σtt̄H+tHggF, Bγγ/BZZ, BWW/BZZ, Bττ/BZZ, and Bbb/BZZ. The fit results are normalized to the SM predictions. The black error bars, blue boxes and yellow boxes show the total, systematic, and statistical uncertainties in the measurements, respectively. The grey bands show the theory uncertainties in the predictions.Reference: Figure 6 in ATLAS-CONF-2018-031

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Run 2 cross sections:
Cross-sections for ggF, VBF, WH, ZH and tt̄H+tH normalized to their SM predictions, measured with the assumption of SM branching fractions. The black error bars, blue boxes and yellow boxes show the total, systematic, and statistical uncertainties in the measurements, respectively. The grey bands indicate the theory uncertainties in the cross-section predictions. Reference: Figure 2 in ATLAS-CONF-2018-031

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Run 1 signal strength in decay modes:
The observed signal strengths and uncertainties for different Higgs boson decay channels and their combination for mH=125.36 GeV. Higgs boson signals corresponding to the same decay channel are combined together for all analyses, assuming SM values for the cross-section ratios of different production processes. The best-fit values are shown by the solid vertical lines. The total ±1σ uncertainties are indicated by green shaded bands, with the individual contributions from the statistical uncertainty (top), the total (experimental and theoretical) systematic uncertainty (middle), and the signal theoretical uncertainty (bottom) on the signal strength shown as horizontal error bars. Reference: Figure 2 in Eur. Phys. J. C (2016) 76:6

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Run 1 signal strength in decay modes (simple version):
The observed and expected signal strengths and uncertainties for different Higgs boson decay channels and their combination for mH=125.36 GeV. Higgs boson signals of the same decay in all analyses are combined together. The best-fit values are shown by the solid vertical lines. The observed total ±1σ uncertainties are indicated by green shaded bands and blue error bars, whereas the expected ±1σ total uncertainties are indicated by red error bars, centered at the expected signal strength of 1. Reference: Auxiliary Figure 7 in Eur. Phys. J. C (2016) 76:6

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Run 1 signal strength in production modes:
The best-fit signal-strength values of different production modes determined from the combined fit to the √s=7 and 8 TeV data. The inner and outer error bars correspond to 68% CL and 95% CL intervals. Total uncertainties combining statistical, experimental and theoretical systematic uncertainties are shown. The fit assumes the SM values of the Higgs boson decay branching ratios for mH=125.36 GeV. Reference: Figure 3 in Eur. Phys. J. C (2016) 76:6

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Run 2 kF vs kV coupling strength:
Observed contours at 68% and 95% CL in the (κF, κV) plane, defined in the asymptotic approximation by -2logΛ = 2.28 and 5.99, respectively, for individual channels and the combined fit. The crosses indicate the best-fit values and the star the SM prediction. Reference: Figure 8 in ATLAS-CONF-2018-031

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Run 2 coupling strength:
Best-fit values and uncertainties of Higgs boson coupling modifiers per particle type with effective photon and gluon couplings and either BBSM = 0 (left), or BBSM included as a free parameter (right). The SM corresponds to BBSM = 0 and all κ parameters set to unity. All parameters except κt are assumed to be positive. In the model with BBSM included as a free parameter, the conditions κW,Z ≤ 1 are also applied and an upper limit on BBSM is reported. Reference: Figure 11 in ATLAS-CONF-2018-031

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Run 2 coupling strength ratios:
Measured ratios of coupling modifiers. The dashed line indicates the SM value of unity for each parameter. Reference: Figure 12 in ATLAS-CONF-2018-031

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Run 2 coupling strengths vs particle mass:
Reduced coupling strength modifiers κFmF/v for fermions (F = t, b, τ, μ) and √κVmV/v for weak gauge bosons (V = W, Z) as a function of their masses mF and mV, respectively, and the vacuum expectation value of the Higgs field v = 246 GeV. The SM prediction for both cases is also shown (dotted line). The couplings modifiers κF and κV are measured assuming no BSM contributions to the Higgs boson decays, and the SM structure of loop processes such as ggF, H→γγ and H→gg. Reference: Figure 10 in ATLAS-CONF-2018-031

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BSM Higgs exclusion in the hMSSM:
Regions of the [mA, tanβ] plane excluded in the hMSSM model via direct searches for heavy Higgs bosons and fits to the measured rates of observed Higgs boson production and decays. Limits are quoted at 95% CL and are indicated for the data (solid lines) and the expectation for the SM Higgs sector (dashed lines). The light shaded or hashed regions indicate the observed exclusions. The cross sections for the Higgs boson production in the hMSSM [Eur. Phys. J. C73, 2650,JHEP 06, 168(2015)] are calculated using up to NNLO QCD corrections for gluon-gluon fusion and b-associated production in the five-flavour scheme as implemented in Sushi [Comput. Phys. Commun., 184:1605-1617,JHEP 12, 015(2015),Phys. Rev. D 68, 013001,Phys. Rev. Lett. 88, 201801]. For b-associated production a cross section in the four-flavour scheme is calculated as described in Refs. [Phys. Rev. D 69, 074027,Phys. Rev. D 70, 074010] and the results are combined with the five-flavour scheme calculation following Ref. [arXiv:1112.3478 (hep-ph)]. The Higgs boson widths and branching ratios have been calculated using HDECAY [Comput. Phys. Commun., 108:56-74]. The procedure for the calculation of the cross sections and the branching ratios follows Ref. [arXiv:1610.07922 (hep-ph)].

Observed limits only
Expected limits only

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BSM Higgs exclusion in the hMSSM (large mA range):
Regions of the [mA, tanβ] plane excluded in the hMSSM model via direct searches for heavy Higgs bosons and fits to the measured rates of observed Higgs boson production and decays. Limits are quoted at 95% CL and are indicated for the data (solid lines) and the expectation for the SM Higgs sector (dashed lines). The light shaded or hashed regions indicate the observed exclusions. The cross sections for the Higgs boson production in the hMSSM [Eur. Phys. J. C73, 2650,JHEP 06, 168(2015)] are calculated using up to NNLO QCD corrections for gluon-gluon fusion and b-associated production in the five-flavour scheme as implemented in Sushi [Comput. Phys. Commun., 184:1605-1617,JHEP 12, 015(2015),Phys. Rev. D 68, 013001,Phys. Rev. Lett. 88, 201801]. For b-associated production a cross section in the four-flavour scheme is calculated as described in Refs. [Phys. Rev. D 69, 074027,Phys. Rev. D 70, 074010] and the results are combined with the five-flavour scheme calculation following Ref. [arXiv:1112.3478 (hep-ph)]. The Higgs boson widths and branching ratios have been calculated using HDECAY [Comput. Phys. Commun., 108:56-74]. The procedure for the calculation of the cross sections and the branching ratios follows Ref. [arXiv:1610.07922 (hep-ph)].

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Summary of HH results:
The 95% C.L. upper limit of Higgs boson pair (HH) production normalized by the SM prediction for gluon–gluon fusion produced HH of σSM (ppHH) = 33.41 fb, which is calculated with mH = 125.09 GeV at next-to-leading order in QCD considering the full top-quark mass dependence in Ref. [Phys. Rev. Lett. 117 (2016) 012001 , Phys. Rev. Lett. 117 (2016) 079901 (Err.)]. The upper limits are obtained separately from several final states of HH decaying to bb̅τ+τ-, bb̅bb̅, bb̅γγ and W+W-γγ.

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ATLAS Collaboration, 2019