#### ${{\mathit H}^{0}}$ SIGNAL STRENGTHS IN DIFFERENT CHANNELS

The ${{\mathit H}^{0}}$ 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( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit x}}{{\mathit x}}$ ) $/$ ($\sigma$ $\cdot{}$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit x}}{{\mathit x}}$ ))$_{{\mathrm {SM}}}$, for the specified mass value of ${{\mathit H}^{0}}$ . 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
 $\bf{ 1.19 \pm0.12}$ OUR AVERAGE
$1.28$ ${}^{+0.17}_{-0.16}$ 1
 2019 AT
CMS ${{\mathit p}}{{\mathit p}}$ , 13 TeV
$1.09$ ${}^{+0.18}_{-0.16}$ 2, 3
 2016 AN
LHC ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.94$ ${}^{+0.85}_{-0.83}$ 4
 2013 M
TEVA ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
• • We do not use the following data for averages, fits, limits, etc. • •
5
 2019 F
ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, cross sections
$2.5$ ${}^{+0.9}_{-0.8}$ 6
 2019 A
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ , 13 TeV
$1.28$ ${}^{+0.18}_{-0.17}$ 7
 2019 AX
CMS ${{\mathit p}}{{\mathit p}}$ , 13 TeV
$1.22$ ${}^{+0.23}_{-0.21}$ 3
 2016 AN
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.90$ ${}^{+0.23}_{-0.21}$ 3
 2016 AN
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
8
 2016 AO
ATLS ${{\mathit p}}{{\mathit p}}$ , 8 TeV, cross sections
$1.18$ $\pm0.16$ ${}^{+0.17}_{-0.14}$ 9
 2016 K
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.09$ ${}^{+0.16}_{-0.15}$ ${}^{+0.17}_{-0.14}$ 10
 2015 AA
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$3.0$ ${}^{+1.3}_{-1.1}$ ${}^{+1.0}_{-0.7}$ 11
 2015 AQ
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 7, 8 TeV
$1.16$ ${}^{+0.16}_{-0.15}$ ${}^{+0.18}_{-0.15}$ 12
 2015 AQ
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.72$ $\pm0.12$ $\pm0.10$ ${}^{+0.12}_{-0.10}$ 13
 2014 G
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.99$ ${}^{+0.31}_{-0.28}$ 14
 2013 AK
ATLS ${{\mathit p}}{{\mathit p}}$ , 7 and 8 TeV
$0.00$ ${}^{+1.78}_{-0.00}$ 15
 2013 L
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$1.90$ ${}^{+1.63}_{-1.52}$ 16
 2013 L
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$1.3$ $\pm0.5$ 17
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
$0.5$ $\pm0.6$ 17
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7 TeV
$1.9$ $\pm0.7$ 17
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 8 TeV
$0.60$ ${}^{+0.42}_{-0.37}$ 18
 2012 N
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
 1 SIRUNYAN 2019AT perform a combine fit to 35.9 fb${}^{-1}$ of data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV.
 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 ${{\mathit W}}{{\mathit H}^{0}}$ production, $5.9$ ${}^{+2.6}_{-2.2}$ for ${{\mathit Z}}{{\mathit H}^{0}}$ production, and $5.0$ ${}^{+1.8}_{-1.7}$ for ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
 5 AABOUD 2019F measure cross-sections times the ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ branching fraction in the ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ channel using 36.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV: $\sigma _{ggF}{\times }$B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) = $11.4$ ${}^{+1.2}_{-1.1}{}^{+1.8}_{-1.7}$ pb and $\sigma _{VBF}{\times }$B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ ) = $0.50$ ${}^{+0.24}_{-0.22}$ $\pm0.17$ pb.
 6 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 ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ and $0.54$ ${}^{+0.31}_{-0.24}{}^{+0.15}_{-0.07}$ pb for ${{\mathit Z}}{{\mathit H}^{0}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ .
 7 SIRUNYAN 2019AX measure the signal strengths, cross sections and so on using gluon fusion, VBF and ${{\mathit V}}{{\mathit H}^{0}}$ production processes with 35.9 fb${}^{-1}$ of data. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 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)).
 8 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 ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ . 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
 9 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.36 GeV.
 10 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.36 GeV.
 11 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.36 GeV.
 12 AAD 2015AQ combine their result on ${{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit H}^{0}}$ production with the results of AAD 2015AA (gluon fusion and vector boson fusion, slightly updated). The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.36 GeV.
 13 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.6 GeV.
 14 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.5 GeV. Superseded by AAD 2015AA.
 15 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
 16 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
 17 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 126 GeV. See also AAD 2012DA.
 18 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 ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.5 GeV. See also CHATRCHYAN 2013Y.
References:
 AABOUD 2019F
PL B789 508 Measurements of gluon-gluon fusion and vector-boson fusion Higgs boson production cross-sections in the $H \to WW^{\ast} \to e\nu\mu\nu$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
PL B798 134949 Measurement of the production cross section for a Higgs boson in association with a vector boson in the $H \to WW^{\ast} \to \ell\nu\ell\nu$ channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
 SIRUNYAN 2019AX
PL B791 96 Measurements of properties of the Higgs boson decaying to a W boson pair in pp collisions at $\sqrt{s}=$ 13 TeV
 SIRUNYAN 2019AT
EPJ C79 421 Combined measurements of Higgs boson couplings in proton?proton collisions at $\sqrt{s}=13\,\text {Te}\text {V}$
EPJ C76 6 Measurements of the Higgs Boson Production and Decay Rates and Coupling Strengths using ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 7 and 8 TeV in the ATLAS Experiment
JHEP 1608 045 Measurements of the Higgs Boson Production and Decay Rates and Constraints on its Couplings from a Combined ATLAS and CMS Analysis of the LHC ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ =7 and 8 TeV
JHEP 1608 104 Measurement of Fiducial Differential Cross Sections of Gluon-Fusion Production of Higgs Bosons Decaying to ${{\mathit W}}$ ${{\mathit W}^{*}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \nu}}{{\mathit \mu}}{{\mathit \nu}}$ with the ATLAS Detector at $\sqrt {s }$ = 8 TeV
JHEP 1508 137 Study of (${{\mathit W}}$ /${{\mathit Z}}$ )${{\mathit H}}$ Production and Higgs Boson Couplings using ${{\mathit H}}$ $\rightarrow$ ${{\mathit W}}{{\mathit W}^{*}}$ Decays with the ATLAS Detector
PR D92 012006 Observation and Measurement of Higgs Boson Decays to ${{\mathit W}}{{\mathit W}^{*}}$ with the ATLAS Detector
 CHATRCHYAN 2014G
JHEP 1401 096 Measurement of Higgs Boson Production and Properties in the ${{\mathit W}}{{\mathit W}}$ Decay Channel with Leptonic Final States
PR D88 052011 Combined Search for the Higgs Boson with the ${D0}$ Experiment