| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $1.07$ ${}^{+0.25}_{-0.31}$ |
1, 2 |
|
ATLS |
| $1.06$ ${}^{+0.25}_{-0.30}$ |
1, 3 |
|
ATLS |
| $1.04$ ${}^{+0.23}_{-0.30}$ |
1, 4 |
|
ATLS |
| $1.12$ $\pm0.20$ |
5, 6 |
|
CMS |
| $1.12$ ${}^{+0.21}_{-0.22}$ |
5, 7 |
|
CMS |
|
1
ATLAS 2022 report combined results (see their Extended Data Table 1) using up to 139 fb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV, assuming ${\mathit m}_{{{\mathit H}}}$ = 125.09 GeV.
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|
2
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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3
${{\mathit B}}_{inv}$ = ${{\mathit B}}_{undetected}$ = 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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4
${{\mathit B}}_{inv}$ 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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|
5
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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6
Only SM particles assume to contribute to the loop-induced processes. See their Fig. 3 right.
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|
7
Coupling strength modifiers including effective photon, ${{\mathit Z}}{{\mathit \gamma}}$ and gluon are measured. See their Fig. 4 left.
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