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

# ${{\boldsymbol Z}}{{\boldsymbol Z}^{*}}$ Final State INSPIRE search

VALUE DOCUMENT ID TECN  COMMENT
$\bf{ 1.14 {}^{+0.15}_{-0.13}}$ OUR AVERAGE
$1.05$ ${}^{+0.15}_{-0.14}$ ${}^{+0.11}_{-0.09}$ 1
 2017 AV
CMS ${{\mathit p}}{{\mathit p}}$ , 13 TeV
$1.29$ ${}^{+0.26}_{-0.23}$ 2, 3
 2016 AN
LHC ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
• • • We do not use the following data for averages, fits, limits, etc. • • •
$1.52$ ${}^{+0.40}_{-0.34}$ 3
 2016 AN
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.04$ ${}^{+0.32}_{-0.26}$ 3
 2016 AN
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.46$ ${}^{+0.35}_{-0.31}$ ${}^{+0.19}_{-0.13}$ 4
 2016 K
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
5
 2016 AR
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV cross sections
$1.44$ ${}^{+0.34}_{-0.31}$ ${}^{+0.21}_{-0.11}$ 6
 2015 F
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
7
 2014 AR
ATLS ${{\mathit p}}{{\mathit p}}$ , 8 TeV, differential cross section
$0.93$ ${}^{+0.26}_{-0.23}$ ${}^{+0.13}_{-0.09}$ 8
 2014 AA
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.43$ ${}^{+0.40}_{-0.35}$ 9
 2013 AK
ATLS ${{\mathit p}}{{\mathit p}}$ , 7 and 8 TeV
$0.80$ ${}^{+0.35}_{-0.28}$ 10
 2013 J
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
$1.2$ $\pm0.6$ 11
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
$1.4$ $\pm1.1$ 11
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7 TeV
$1.1$ $\pm0.8$ 11
 2012 AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 8 TeV
$0.73$ ${}^{+0.45}_{-0.33}$ 12
 2012 N
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
1  SIRUNYAN 2017AV use 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted signal strength, obtained from the analysis of ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ ( ${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ ) decays, is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.09 GeV. The signal strengths for different production modes are given in their Table 3. The fiducial and differential cross sections are shown in their Fig. 10.
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 $1.13$ ${}^{+0.34}_{-0.31}$ for gluon fusion and $0.1$ ${}^{+1.1}_{-0.6}$ for vector boson fusion.
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  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.
5  KHACHATRYAN 2016AR use data of 5.1 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.7 fb${}^{-1}$ at 8 TeV. The fiducial cross sections for the production of 4 leptons via ${{\mathit H}^{0}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ decays are measured to be $0.56$ ${}^{+0.67}_{-0.44}{}^{+0.21}_{-0.06}$ fb at 7 TeV and $1.11$ ${}^{+0.41}_{-0.35}{}^{+0.14}_{-0.10}$ fb at 8 TeV in their fiducial region (Table 2). The differential cross sections at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV are also shown in Figs. 4 and 5. The results are given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV.
6  AAD 2015F 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. The signal strength for the gluon fusion production mode is $1.66$ ${}^{+0.45}_{-0.41}{}^{+0.25}_{-0.15}$, while the signal strength for the vector boson fusion production mode is $0.26$ ${}^{+1.60}_{-0.91}{}^{+0.36}_{-0.23}$.
7  AAD 2014AR measure the cross section for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ using 20.3 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. They give ${{\mathit \sigma}}\cdot{}{{\mathit B}}$ = $2.11$ ${}^{+0.53}_{-0.47}$ $\pm0.08$ fb in their fiducial region, where $1.30$ $\pm0.13$ fb is expected in the Standard Model for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.4 GeV. Various differential cross sections are also given, which are in agreement with the Standard Model expectations.
8  CHATRCHYAN 2014AA use 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 19.7 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.6 GeV. The signal strength for the gluon fusion and ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}}$ production mode is $0.80$ ${}^{+0.46}_{-0.36}$, while the signal strength for the vector boson fusion and ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ production mode is $1.7$ ${}^{+2.2}_{-2.1}$.
9  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.
10  CHATRCHYAN 2013J obtain results based on ${{\mathit Z}}$ ${{\mathit Z}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ final states in 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 12.2 fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.8 GeV. Superseded by CHATRCHYAN 2014AA.
11  AAD 2012AI obtain results based on $4.7 - 4.8$ 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.
12  CHATRCHYAN 2012N obtain results based on $4.9 - 5.1$ fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and $5.1 - 5.3$ fb${}^{-1}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. An excess of events over background with a local significance of 5.0 $\sigma$ is observed at about ${\mathit m}_{{{\mathit H}^{0}}}$ = 125 GeV. The quoted signal strengths are given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.5 GeV. See also CHATRCHYAN 2012BY and CHATRCHYAN 2013Y.
References:
 SIRUNYAN 2017AV
JHEP 1711 047 Measurements of Properties of the Higgs Boson Decaying into the Four-Lepton Final State in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV
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
 KHACHATRYAN 2016AR
JHEP 1604 005 Measurement of Differential and Integrated Fiducial Cross Sections for Higgs Boson Production in the Four-Lepton Decay Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV
PR D91 012006 Measurements of Higgs Boson Production and Couplings in the Four-Lepton Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at Center-of-Mass Energies of 7 and 8 TeV with the ATLAS Detector
PL B738 234 Fiducial and Differential Cross Sections of Higgs boson Production Measured in the Four-Lepton Decay Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS detector
 CHATRCHYAN 2014AA
PR D89 092007 Measurement of the Properties of a Higgs Boson in the Four-Lepton Final State
PRL 110 081803 On the Mass and Spin-Parity of the Higgs Boson Candidate via its Decays to ${{\mathit Z}}$ Boson Pairs
JHEP 1306 081 Observation of a New Boson with Mass Near 125 GeV in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 and 8 TeV