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

${{\boldsymbol \gamma}}{{\boldsymbol \gamma}}$ Final State INSPIRE search

VALUE DOCUMENT ID TECN  COMMENT
$\bf{ 1.16 \pm0.18}$ OUR AVERAGE
$1.14$ ${}^{+0.19}_{-0.18}$ 1, 2
AAD
2016AN
LHC ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$5.97$ ${}^{+3.39}_{-3.12}$ 3
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. • • •
$1.14$ ${}^{+0.27}_{-0.25}$ 2
AAD
2016AN
ATLS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.11$ ${}^{+0.25}_{-0.23}$ 2
AAD
2016AN
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
4
KHACHATRYAN
2016B
CMS ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}^{*}}{{\mathit \gamma}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \gamma}}$
5
KHACHATRYAN
2016G
CMS differential cross section
$1.17$ $\pm0.23$ ${}^{+0.10}_{-0.08}$ ${}^{+0.12}_{-0.08}$ 6
AAD
2014BC
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
7
AAD
2014BJ
ATLS ${{\mathit p}}{{\mathit p}}$ , 8 TeV, differential cross section
$1.14$ $\pm0.21$ ${}^{+0.09}_{-0.05}$ ${}^{+0.13}_{-0.09}$ 8
KHACHATRYAN
2014P
CMS ${{\mathit p}}{{\mathit p}}$ , 7, 8 TeV
$1.55$ ${}^{+0.33}_{-0.28}$ 9
AAD
2013AK
ATLS ${{\mathit p}}{{\mathit p}}$ , 7 and 8 TeV
$7.81$ ${}^{+4.61}_{-4.42}$ 10
AALTONEN
2013L
CDF ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$4.20$ ${}^{+4.60}_{-4.20}$ 11
ABAZOV
2013L
D0 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 1.96 TeV
$1.8$ $\pm0.5$ 12
AAD
2012AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
$2.2$ $\pm0.7$ 12
AAD
2012AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7 TeV
$1.5$ $\pm0.6$ 12
AAD
2012AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 8 TeV
$1.54$ ${}^{+0.46}_{-0.42}$ 13
CHATRCHYAN
2012N
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , 7, 8 TeV
1  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 $1.10$ ${}^{+0.23}_{-0.22}$ for gluon fusion, $1.3$ $\pm0.5$ for vector boson fusion, $0.5$ ${}^{+1.3}_{-1.2}$ for ${{\mathit W}}{{\mathit H}^{0}}$ production, $0.5$ ${}^{+3.0}_{-2.5}$ for ${{\mathit Z}}{{\mathit H}^{0}}$ production, and $2.2$ ${}^{+1.6}_{-1.3}$ for ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ production.
2  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.
3  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.
4  KHACHATRYAN 2016B search for ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}^{*}}{{\mathit \gamma}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit \gamma}}$ and ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}{{\mathit \gamma}}$ (with m( ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ ) $<$ 20 GeV) in 19.7 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV. An upper limit of 6.7 times the Standard Model expectation is obtained at 95$\%$ CL. See their Fig. 6 for limits on individual channels.
5  KHACHATRYAN 2016G measure fiducial and differential cross sections of the process ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with 19.7 fb${}^{-1}$. See their Figs. $4 - 6$ and Table 1 for data.
6  AAD 2014BC 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 last uncertainty in the measurement is theory systematics. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 125.4 GeV. The signal strengths for the individual production modes are: $1.32$ $\pm0.38$ for gluon fusion, $0.8$ $\pm0.7$ for vector boson fusion, $1.0$ $\pm1.6$ for ${{\mathit W}}{{\mathit H}^{0}}$ production, $0.1$ ${}^{+3.7}_{-0.1}$ for ${{\mathit Z}}{{\mathit H}^{0}}$ production, and $1.6$ ${}^{+2.7}_{-1.8}$ for ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ production.
7  AAD 2014BJ measure fiducial and differential cross sections of the process ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}^{0}}{{\mathit X}}$ , ${{\mathit H}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with 20.3 fb${}^{-1}$. See their Table 3 and Figs. $3 - 12$ for data.
8  KHACHATRYAN 2014P 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 last uncertainty in the measurement is theory systematics. The quoted signal strength is given for ${\mathit m}_{{{\mathit H}^{0}}}$ = 124.7 GeV. The signal strength for the gluon fusion and ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}}$ production mode is $1.13$ ${}^{+0.37}_{-0.31}$, while the signal strength for the vector boson fusion and ${{\mathit W}}{{\mathit H}^{0}}$ , ${{\mathit Z}}{{\mathit H}^{0}}$ production mode is $1.16$ ${}^{+0.63}_{-0.58}$.
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  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.
11  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.
12  AAD 2012AI obtain results based on 4.8 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV and 5.9 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.
13  CHATRCHYAN 2012N obtain results based on 5.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$=7 TeV and 5.3 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:
AAD 2016AN
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 2016G
EPJ C76 13 Measurement of Differential Cross Sections for Higgs Boson Production in the Diphoton Decay Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2016B
PL B753 341 Search for a Higgs Boson Decaying into ${{\mathit \gamma}^{*}}$ ${{\mathit \gamma}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}{{\mathit \gamma}}$ with Low Dilepton Mass in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
AAD 2014BC
PR D90 112015 Measurement of Higgs Boson Production in the Diphoton Decay Channel in ${{\mathit p}}{{\mathit p}}$ Collisions at Center-of-Mass Energies of 7 and 8 TeV with the ATLAS Detector
AAD 2014BJ
JHEP 1409 112 Measurements of Fiducial and Differential Cross Sections for Higgs Boson Production in the Diphoton Decay Channel at $\sqrt {s }$ = 8 TeV with ATLAS
KHACHATRYAN 2014P
EPJ C74 3076 Observation of the Diphoton Decay of the Higgs Boson and Measurement of its Properties
AAD 2013AK
PL B726 88 Measurements of Higgs Boson Production and Couplings in Diboson Final States with the ATLAS Detector at the LHC
AALTONEN 2013M
PR D88 052014 Higgs Boson Studies at the Tevatron
AALTONEN 2013L
PR D88 052013 Combination of Searches for the Higgs Boson Using the Full CDF Data Set
ABAZOV 2013L
PR D88 052011 Combined Search for the Higgs Boson with the ${D0}$ Experiment
AAD 2012AI
PL B716 1 Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector at the LHC
CHATRCHYAN 2012N
PL B716 30 Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC
AAD 2012DA
SCI 338 1576 A Particle Consistent with the Higgs Boson Observed with the ATLAS Detector at the Large Hadron Collider
CHATRCHYAN 2013Y
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