| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $0.65 < \vert {{\mathit \kappa}_{{{b}}}}\vert < 1.37$ |
95 |
1 |
|
ATLS |
| $\text{-1.09 to -0.86 OR 0.81 to 1.09}$ |
95 |
2 |
|
ATLS |
|
|
3 |
|
ATLS |
| $-1.1\text{ to }1.1 $ |
95 |
4 |
|
CMS |
| $0.90$ $\pm0.11$ |
|
5, 6 |
|
ATLS |
| $0.89$ $\pm0.11$ |
|
5, 7 |
|
ATLS |
| $0.82$ ${}^{+0.09}_{-0.08}$ |
|
5, 8 |
|
ATLS |
| $1.02$ ${}^{+0.15}_{-0.17}$ |
|
9, 10 |
|
CMS |
| $0.99$ ${}^{+0.17}_{-0.16}$ |
|
9, 11 |
|
CMS |
|
1
AAD 2025Y present measurements of ${{\mathit V}}{{\mathit H}}$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ and ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$ (${{\mathit V}}$ = ${{\mathit W}}$ , ${{\mathit Z}}$) using 140 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted value is obtained assuming ${{\mathit \kappa}_{{{c}}}}$ = 1, all other couplings to their SM predictions, and only SM decays.
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2
AAD 2023C combine results of ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ and ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$) using 139 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The Higgs boson transverse momentum (${{\mathit p}}{}^{H}_{T}$) distribution constrains $\kappa _{b}$ and $\kappa _{c}$, assuming other couplings fixed to the SM values. The $\kappa _{b}$ is obtained using the ${{\mathit p}}{}^{H}_{T}$ shape and normalisation. Other cases are given in their Tables 6 and 7.
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3
AAD 2023CD search for ${{\mathit H}}$ $\rightarrow$ ${{\mathit \Upsilon}{(nS)}}{{\mathit \gamma}}$, ${{\mathit \Upsilon}{(nS)}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ (n=1,2,3) with 138 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. They interpret the ${{\mathit H}}$ $\rightarrow$ ${{\mathit \Upsilon}{(nS)}}{{\mathit \gamma}}$ search to constraint the bottom Yukawa coupling by comparing to ${{\mathit H}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$. An observed 95$\%$ CL interval of (-37, 40) is obtained for ${{\mathit \kappa}_{{{b}}}}/{{\mathit \kappa}_{{{\gamma}}}}$.
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4
HAYRAPETYAN 2023 measure the cross sections for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$) using 138 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The $\kappa _{b}$ is obtained from the $p_T$ differential cross section of the ggF production employing the dependence of the branching fraction on $\kappa _{b}$ and $\kappa _{c}$.
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5
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139fb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV, assuming ${\mathit m}_{{{\mathit H}}}$ = 125.09 GeV.
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6
All modifiers ($\kappa $) $>$ 0, and $\kappa _{c}$ = $\kappa _{t}$ (${{\mathit B}}_{inv}$ = ${{\mathit B}}_{undetected}$ = 0) are assumed. Only SM particles assume to contribute to the loop-induced processes. See their Fig. 5, which shows both $\kappa _{c}$ = $\kappa _{t}$ and $\kappa _{c}$ floating.
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7
${{\mathit B}}_{inv}$ = ${{\mathit B}}_{undetected}$ = 0 is assumed. Coupling strength modifiers including effective photon, ${{\mathit Z}}{{\mathit \gamma}}$ and gluon are measured. See their Fig. 6.
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8
${{\mathit B}}_{inv}$ floating, ${{\mathit B}}_{undetected}{}\geq{}$ 0, and $\kappa _{V}{}\leq{}$ 1 are assumed. Coupling strength modifiers including effective photon, ${{\mathit Z}}{{\mathit \gamma}}$ and gluon are measured. See their Fig. 6.
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9
CMS 2022 report combined results (see their Extended Data Table 2) using up to 138 fb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV, assuming ${\mathit m}_{{{\mathit H}}}$ = 125.38 GeV.
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10
Only SM particles assume to contribute to the loop-induced processes. See their Fig. 3 right.
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11
Coupling strength modifiers including effective photon, ${{\mathit Z}}{{\mathit \gamma}}$ and gluon are measured. See their Fig. 4 left.
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