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${{\mathit H}}$ SIGNAL STRENGTHS IN DIFFERENT CHANNELS

The ${{\mathit H}}$ signal strength in a particular final state ${{\mathit x}}{{\mathit x}}$ is given by the cross section times branching ratio in this channel normalized to the Standard Model (SM) value, $\sigma $ $\cdot{}$ B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit x}}{{\mathit x}}$ ) $/$ ($\sigma $ $\cdot{}$ B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit x}}{{\mathit x}}$ ))$_{{\mathrm {SM}}}$, for the specified mass value of ${{\mathit H}}$. For the SM predictions, see DITTMAIER 2011 , DITTMAIER 2012 , and HEINEMEYER 2013A. Results for fiducial and differential cross sections are also listed below.

${{\mathit W}}{{\mathit W}^{*}}$ Final State

VALUE

DOCUMENT ID

TECN

COMMENT

$\bf{ 1.00 \pm0.08}$

OUR AVERAGE

$0.97$ $\pm0.09$

CMS

${{\mathit p}}{{\mathit p}}$ , 13 TeV

$1.09$ ${}^{+0.18}_{-0.16}$

LHC

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

$0.94$ ${}^{+0.85}_{-0.83}$

TEVA

${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 1.96 TeV

• • We do not use the following data for averages, fits, limits, etc. • •

$0.5$ $\pm0.4$ ${}^{+0.7}_{-0.6}$

ATLS

${{\mathit p}}{{\mathit p}}$ , ${{\mathit W}}{{\mathit W}^{*}}$ ( $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ ) + 2 ${{\mathit j}}$ , 13 TeV

ATLS

${{\mathit p}}{{\mathit p}}$ , ${{\mathit W}}{{\mathit W}^{*}}$ ( $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ ) + 2 ${{\mathit j}}$ , 13 TeV

ATLS

${{\mathit p}}{{\mathit p}}$ , 13 TeV, cross sections

$2.5$ ${}^{+0.9}_{-0.8}$

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit W}}$ $/$ ${{\mathit H}}{{\mathit Z}}$ , ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ , 13 TeV

$1.28$ ${}^{+0.17}_{-0.16}$

CMS

${{\mathit p}}{{\mathit p}}$ , 13 TeV

$1.28$ ${}^{+0.18}_{-0.17}$

CMS

${{\mathit p}}{{\mathit p}}$ , 13 TeV

$1.22$ ${}^{+0.23}_{-0.21}$

ATLS

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

$0.90$ ${}^{+0.23}_{-0.21}$

CMS

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

ATLS

${{\mathit p}}{{\mathit p}}$ , 8 TeV, cross sections

$1.18$ $\pm0.16$ ${}^{+0.17}_{-0.14}$

ATLS

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

$1.09$ ${}^{+0.16}_{-0.15}$ ${}^{+0.17}_{-0.14}$

ATLS

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

$3.0$ ${}^{+1.3}_{-1.1}$ ${}^{+1.0}_{-0.7}$

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 7, 8 TeV

$1.16$ ${}^{+0.16}_{-0.15}$ ${}^{+0.18}_{-0.15}$

ATLS

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

$0.72$ $\pm0.12$ $\pm0.10$ ${}^{+0.12}_{-0.10}$

CMS

${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV

$0.99$ ${}^{+0.31}_{-0.28}$

ATLS

${{\mathit p}}{{\mathit p}}$ , 7 and 8 TeV

$0.00$ ${}^{+1.78}_{-0.00}$

CDF

${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 1.96 TeV

$1.90$ ${}^{+1.63}_{-1.52}$

D0

${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 1.96 TeV

$1.3$ $\pm0.5$

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 7, 8 TeV

$0.5$ $\pm0.6$

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 7 TeV

$1.9$ $\pm0.7$

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 8 TeV

$0.60$ ${}^{+0.42}_{-0.37}$

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit X}}$ , 7, 8 TeV

¹	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. See their Fig. 2 right.

²

AAD 2016AN perform fits to the ATLAS and CMS data at $\mathit E_{{\mathrm {cm}}}$ = 7 and 8 TeV. The signal strengths for individual production processes are $0.84$ $\pm0.17$ for gluon fusion, $1.2$ $\pm0.4$ for vector boson fusion, $1.6$ ${}^{+1.2}_{-1.0}$ for ${{\mathit W}}{{\mathit H}}$ production, $5.9$ ${}^{+2.6}_{-2.2}$ for ${{\mathit Z}}{{\mathit H}}$ production, and $5.0$ ${}^{+1.8}_{-1.7}$ for ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}}$ production.

³	AAD 2016AN: In the fit, relative production cross sections are fixed to those in the Standard Model. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.09 GeV.

⁴

AALTONEN 2013M combine all Tevatron data from the CDF and D0 Collaborations with up to 10.0 fb${}^{-1}$ and 9.7 fb${}^{-1}$, respectively, of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.

⁵	AAD 2022V measure the signal strength for ggF+2jets with 36.1 fb${}^{-1}$ data at 13 TeV.

⁶

AAD 2022V probe the Higgs couplings to longitudinally and transversely polarized ${{\mathit W}}$ and ${{\mathit Z}}$ using VBF ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ plus two jets) with 36.1 fb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The ratios of the polarization-dependent couplings $\mathit g_{ {{\mathit H}} {{\mathit V}_{{{L}}}} {{\mathit V}_{{{L}}}} }$ and $\mathit g_{ {{\mathit H}} {{\mathit V}_{{{T}}}} {{\mathit V}_{{{T}}}} }$ to the Higgs-${{\mathit V}}$ coupling predicted by the SM, ${{\mathit a}_{{{L}}}}$ = $\mathit g_{ {{\mathit H}} {{\mathit V}_{{{L}}}} {{\mathit V}_{{{L}}}} }/\mathit g{}^{{\mathrm {SM}}}_{ HVV}$ and ${{\mathit a}_{{{T}}}}$ = $\mathit g_{ {{\mathit H}} {{\mathit V}_{{{T}}}} {{\mathit V}_{{{T}}}} }/\mathit g{}^{{\mathrm {SM}}}_{ HVV}$ are measured to be $0.91$ ${}^{+0.10}_{-0.18}{}^{+0.09}_{-0.17}$ and $1.2$ $\pm0.4$ ${}^{+0.2}_{-0.3}$, respectively, assuming the standard ${{\mathit H}}{{\mathit g}}{{\mathit g}}$ coupling. These measurements are translated into pseudo-observables of ${{\mathit \kappa}_{{{VV}}}}$ and ${{\mathit \epsilon}_{{{VV}}}}$: ${{\mathit \kappa}_{{{VV}}}}$ = $0.91$ ${}^{+0.10}_{-0.18}{}^{+0.09}_{-0.17}$ and ${{\mathit \epsilon}_{{{VV}}}}$ = $0.13$ ${}^{+0.28}_{-0.20}{}^{+0.08}_{-0.10}$, where ${{\mathit \kappa}_{{{VV}}}}$ = 1 and ${{\mathit \epsilon}_{{{VV}}}}$ = 0 for the SM. See their Tables 9 and 10.

⁷

AABOUD 2019F measure cross-sections times the ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ branching fraction in the ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ channel using 36.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV: $\sigma _{ggF}{\times }$B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) = $11.4$ ${}^{+1.2}_{-1.1}{}^{+1.8}_{-1.7}$ pb and $\sigma _{VBF}{\times }$B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) = $0.50$ ${}^{+0.24}_{-0.22}$ $\pm0.17$ pb.

⁸

AAD 2019A use 36.1 fb${}^{-1}$ data at 13 TeV. The cross section times branching fraction values are measured to be $0.67$ ${}^{+0.31}_{-0.27}{}^{+0.18}_{-0.14}$ pb for ${{\mathit W}}{{\mathit H}}$ , ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ and $0.54$ ${}^{+0.31}_{-0.24}{}^{+0.15}_{-0.07}$ pb for ${{\mathit Z}}{{\mathit H}}$ , ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ .

⁹	SIRUNYAN 2019AT perform a combine fit to 35.9 fb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV.

¹⁰

SIRUNYAN 2019AX measure the signal strengths, cross sections and so on using gluon fusion, VBF and ${{\mathit V}}{{\mathit H}}$ production processes with 35.9 fb${}^{-1}$ of data. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.09 GeV. Signal strengths for each production process is found in their Fig. 9. Measured cross sections and ratios to the SM predictions in the stage-0 simplified template cross section framework are shown in their Fig. 10. ${{\mathit \kappa}_{{{F}}}}$ = $1.52$ ${}^{+0.48}_{-0.41}$ and ${{\mathit \kappa}_{{{V}}}}$ = $1.10$ $\pm0.08$ are obtained (see their Fig. 11 (right)).

¹¹

AAD 2016AO measure fiducial total and differential cross sections of gluon fusion process at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with 20.3 fb${}^{-1}$ using ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ . The measured fiducial total cross section is $36.0$ $\pm9.7$ fb in their fiducial region (Table 7). See their Fig. 6 for fiducial differential cross sections. The results are given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.

¹²	AAD 2016K use up to 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.36 GeV.

¹³

AAD 2015AA use 4.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The signal strength for the gluon fusion and vector boson fusion mode is $1.02$ $\pm0.19$ ${}^{+0.22}_{-0.18}$ and $1.27$ ${}^{+0.44}_{-0.40}{}^{+0.30}_{-0.21}$, respectively. The quoted signal strengths are given for ${\mathit m}_{{{\mathit H}}}$ = 125.36 GeV.

¹⁴	AAD 2015AQ use 4.5 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.36 GeV.

¹⁵	AAD 2015AQ combine their result on ${{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit H}}$ production with the results of AAD 2015AA (gluon fusion and vector boson fusion, slightly updated). The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.36 GeV.

¹⁶

CHATRCHYAN 2014G use 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.4 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The last uncertainty in the measurement is theory systematics. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.6 GeV.

¹⁷	AAD 2013AK use 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 20.7 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.5 GeV. Superseded by AAD 2015AA.

¹⁸	AALTONEN 2013L combine all CDF results with $9.45 - 10.0$ fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.

¹⁹	ABAZOV 2013L combine all D0 results with up to 9.7 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.

²⁰	AAD 2012AI obtain results based on 4.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 5.8 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strengths are given for ${\mathit m}_{{{\mathit H}}}$ = 126 GeV. See also AAD 2012DA.

²¹

CHATRCHYAN 2012N obtain results based on 4.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 5.1 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}}}$ = 125.5 GeV. See also CHATRCHYAN 2013Y.

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