${{\boldsymbol H}^{0}}$ 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.

${{\boldsymbol b}}{{\overline{\boldsymbol b}}}$ Final State INSPIRE search

VALUE DOCUMENT ID TECN  COMMENT
$\bf{ 1.04 \pm0.13}$ OUR AVERAGE
$1.12$ $\pm0.29$ 1
SIRUNYAN
2019AT
 CMS ${{\mathit p}}{{\mathit p}}$ , 13 TeV
$1.16$ ${}^{+0.27}_{-0.25}$ 2
AABOUD
2018BN
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 13 TeV, 79.8 fb${}^{-1}$
$1.06$ $\pm0.26$ 3
SIRUNYAN
2018DB
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 13 TeV, 77.2 fb${}^{-1}$
$0.70$ ${}^{+0.29}_{-0.27}$ 4, 5
AAD
2016AN
 LHC ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.59$ ${}^{+0.69}_{-0.72}$ 6
AALTONEN
2013M
 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. • • •
7
AABOUD
2019U
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 13 TeV, cross sections
$0.98$ ${}^{+0.22}_{-0.21}$ 8
AABOUD
2018BN
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 7, 8, 13 TeV
$1.01$ $\pm0.20$ 9
AABOUD
2018BN
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ggF, VBF, ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ 7, 8, 13 TeV
$2.5$ ${}^{+1.4}_{-1.3}$ 10, 11
AABOUD
2018BQ
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , VBF, ggF, ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ , 13 TeV
$3.0$ ${}^{+1.7}_{-1.6}$ 10, 12
AABOUD
2018BQ
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , VBF, 13 TeV
13
AALTONEN
2018C
 CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$1.19$ ${}^{+0.40}_{-0.38}$ 14
SIRUNYAN
2018AE
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 13 TeV
$1.06$ ${}^{+0.31}_{-0.29}$ 15
SIRUNYAN
2018AE
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 7, 8, 13 TeV
$1.01$ $\pm0.22$ 16
SIRUNYAN
2018DB
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit H}^{0}}{{\mathit Z}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 7, 8, 13 TeV
$1.04$ $\pm0.20$ 17
SIRUNYAN
2018DB
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ggF, VBF, ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ 7, 8, 13 TeV
$2.3$ ${}^{+1.8}_{-1.6}$ 18
SIRUNYAN
2018E
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , boosted, 13 TeV
$1.20$ ${}^{+0.24}_{-0.23}$ ${}^{+0.34}_{-0.28}$ 19
AABOUD
2017BA
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 13 TeV, 36.1 fb${}^{-1}$
$0.90$ $\pm0.18$ ${}^{+0.21}_{-0.19}$ 20
AABOUD
2017BA
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ , 7, 8, 13 TeV
$-0.8$ $\pm1.3$ ${}^{+1.8}_{-1.9}$ 21
AABOUD
2016X
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , VBF, 8 TeV
$0.62$ $\pm0.37$ 5
AAD
2016AN
 ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.81$ ${}^{+0.45}_{-0.43}$ 5
AAD
2016AN
 CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.63$ ${}^{+0.31}_{-0.30}$ ${}^{+0.24}_{-0.23}$ 22
AAD
2016K
 ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$0.52$ $\pm0.32$ $\pm0.24$ 23
AAD
2015G
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 7, 8 TeV
$2.8$ ${}^{+1.6}_{-1.4}$ 24
KHACHATRYAN
2015Z
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , VBF, 8 TeV
$1.03$ ${}^{+0.44}_{-0.42}$ 25
KHACHATRYAN
2015Z
 CMS ${{\mathit p}}{{\mathit p}}$ , 8 TeV, combined
$1.0$ $\pm0.5$ 26
CHATRCHYAN
2014AI
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 7, 8 TeV
$1.72$ ${}^{+0.92}_{-0.87}$ 27
AALTONEN
2013L
 CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$1.23$ ${}^{+1.24}_{-1.17}$ 28
ABAZOV
2013L
 D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$0.5$ $\pm2.2$ 29
AAD
2012AI
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 7 TeV
30
AALTONEN
2012T
 TEVA ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 1.96 TeV
$0.48$ ${}^{+0.81}_{-0.70}$ 31
CHATRCHYAN
2012N
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit W}}$ $/$ ${{\mathit Z}}{{\mathit X}}$ , 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  AABOUD 2018BN search for ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ( ${{\mathit V}}$ = ${{\mathit W}}$ , ${{\mathit Z}}$ ) using 79.8 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength corresponds to a significance of 4.9 standard deviations and is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
3  SIRUNYAN 2018DB search for ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ( ${{\mathit V}}$ = ${{\mathit W}}$ , ${{\mathit Z}}$ ) using 77.2 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength corresponds to a significance of 4.4 standard deviations and is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.09 GeV.
4  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 $1.0$ $\pm0.5$ for ${{\mathit W}}{{\mathit H}^{0}}$ production, $0.4$ $\pm0.4$ for ${{\mathit Z}}{{\mathit H}^{0}}$ production, and $1.1$ $\pm1.0$ for ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ production.
5  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.
6  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.
7  AABOUD 2019U measure cross sections of ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ production as a function of the gauge boson transverse momentum using data of 79.8 fb${}^{-1}$. The kinematic fiducial volumes used is based on the simplified template cross section framework (reduced stage-1). See their Table 3 and Fig. 3.
8  AABOUD 2018BN combine results of 79.8 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV with results of ${{\mathit V}}{{\mathit H}^{0}}$ at $\mathit E_{{\mathrm {cm}}}$ = 7 and 8 TeV.
9  AABOUD 2018BN combine results of ${{\mathit V}}{{\mathit H}^{0}}$ at $\mathit E_{{\mathrm {cm}}}$ = 7, 8 and 13 TeV with results of VBF (+gluon fusion) and ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ at $\mathit E_{{\mathrm {cm}}}$ = 7, 8, and 13 TeV to perform a search for the ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ decay. The quoted signal strength assumes a SM production strength and corresponds to a significance of 5.4 standard deviations.
10  AABOUD 2018BQ search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ produced through vector-boson fusion (VBF) and VBF+${{\mathit \gamma}}$ with 30.6 fb${}^{-1}$ ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
11  The signal strength is measured including all production modes (VBF, ggF, ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ ).
12  The signal strength is measured for VBF-only and others (ggF, ${{\mathit V}}{{\mathit H}^{0}}$ , ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ ) are constrained to Standard Model expectations with uncertainties described in their Section VIII B.
13  AALTONEN 2018C use 5.4 fb${}^{-1}$ of ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV. The upper limit at 95$\%$ CL on ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ is 33 times the SM predicion, which corresponds to a cross section of 40.6 pb.
14  SIRUNYAN 2018AE use 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength corresponds to 3.3 standard deviations and is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.09 GeV.
15  SIRUNYAN 2018AE combine the result of 35.9 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV with the results obtained from data of up to 5.1 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 18.9 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV (CHATRCHYAN 2014AI and KHACHATRYAN 2015Z). The quoted signal strength corresponds to 3.8 standard deviations and is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.09 GeV.
16  SIRUNYAN 2018DB combine the result of 77.2 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV with the results obtained from data of up to 5.1 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 18.9 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength corresponds to a significance of 4.8 standard deviations and is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.09 GeV.
17  SIRUNYAN 2018DB combine results of 77.2 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV with results of gluon fusion (ggF), VBF and ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV, 8 TeV and 13 TeV to perform a search for the ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ decay. The quoted signal strength assumes a SM production strength and corresponds to a significance of 5.6 standard deviations and is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.09 GeV.
18  SIRUNYAN 2018E use 35.9 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. They measure ${{\mathit \sigma}}\cdot{}{{\mathit B}}$ for gluon fusion production of ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ with $p_T>$450 GeV, $\vert \eta \vert <$2.5 to be $74$ $\pm48$ ${}^{+17}_{-10}$ fb.
19  AABOUD 2017BA use 36.1 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. They give ${\mathit \sigma (}$W H${)}\cdot{}{{\mathit B}}$( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ) = $1.08$ ${}^{+0.54}_{-0.47}$ pb and ${\mathit \sigma (}$Z H${)}\cdot{}{{\mathit B}}$( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ) = $0.57$ ${}^{+0.26}_{-0.23}$ pb.
20  AABOUD 2017BA combine 7, 8 and 13 TeV analyses. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
21  AABOUD 2016X search for vector-boson fusion production of ${{\mathit H}^{0}}$ decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ in 20.2 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
22  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.
23  AAD 2015G use 4.7 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.
24  KHACHATRYAN 2015Z search for vector-boson fusion production of ${{\mathit H}^{0}}$ decaying to ${{\mathit b}}{{\overline{\mathit b}}}$ in up to 19.8 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
25  KHACHATRYAN 2015Z combined vector boson fusion, ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ production, and ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ production results. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
26  CHATRCHYAN 2014AI use up to 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and up to 18.9 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. See also CHATRCHYAN 2014AJ.
27  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.
28  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.
29  AAD 2012AI obtain results based on $4.6 - 4.8$ fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV. The quoted signal strengths are given in their Fig. 10 for ${\mathit m}_{{{\mathit H}^{0}}}$ = 126 GeV. See also Fig. 13 of AAD 2012DA.
30  AALTONEN 2012T combine AALTONEN 2012Q, AALTONEN 2012R, AALTONEN 2012S, ABAZOV 2012O, ABAZOV 2012P, and ABAZOV 2012K. An excess of events over background is observed which is most significant in the region ${\mathit m}_{{{\mathit H}^{0}}}$ = $120 - 135$ GeV, with a local significance of up to 3.3 $\sigma $. The local significance at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV is 2.8 $\sigma $, which corresponds to (${\mathit \sigma (}$ ${{\mathit H}^{0}}{{\mathit W}}{)}$ + ${\mathit \sigma (}$ ${{\mathit H}^{0}}{{\mathit Z}}{)}$) $\cdot{}$ B( ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ ) = ($0.23$ ${}^{+0.09}_{-0.08}$) pb, compared to the Standard Model expectation at ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV of $0.12$ $\pm0.01$ pb. Superseded by AALTONEN 2013M.
31  CHATRCHYAN 2012N obtain results based on 5.0 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.
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AABOUD 2019U
JHEP 1905 141 Measurement of VH, $ \mathrm{H}\to \mathrm{b}\overline{\mathrm{b}} $ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
SIRUNYAN 2019AT
EPJ C79 421 Combined measurements of Higgs boson couplings in proton?proton collisions at $\sqrt{s}=13\,\text {Te}\text {V} $
AABOUD 2018BN
PL B786 59 Observation of $H \rightarrow b\bar{b}$ decays and $VH$ production with the ATLAS detector
AABOUD 2018BQ
PR D98 052003 Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\sqrt{s} = 13$ $\mathrm{TeV}$ $pp$ collisions with the ATLAS detector
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SIRUNYAN 2018AE
PL B780 501 Evidence for the Higgs boson decay to a bottom quark?antiquark pair
SIRUNYAN 2018DB
PRL 121 121801 Observation of Higgs boson decay to bottom quarks
SIRUNYAN 2018E
PRL 120 071802 Inclusive Search for a Highly Boosted Higgs Boson Decaying to a Bottom Quark-Antiquark Pair
AABOUD 2017BA
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AABOUD 2016X
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AAD 2016AN
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AAD 2015G
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KHACHATRYAN 2015Z
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AALTONEN 2013L
PR D88 052013 Combination of Searches for the Higgs Boson Using the Full CDF Data Set
AALTONEN 2013M
PR D88 052014 Higgs Boson Studies at the Tevatron
ABAZOV 2013L
PR D88 052011 Combined Search for the Higgs Boson with the ${D0}$ Experiment
AAD 2012AI
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AALTONEN 2012T
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