OTHER ${{\mathit H}}$ PRODUCTION PROPERTIES

${{\mathit H}}$ Production Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV

INSPIRE   PDGID:
S126A02
Assumes ${\mathit m}_{{{\mathit H}}}$ = 125 GeV
VALUE (pb) DOCUMENT ID TECN  COMMENT
$\bf{ 56.9 \pm3.4}$ OUR AVERAGE
$58$ $\pm4$ $\pm4$ 1
AAD
2022N
 ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit \gamma}}{{\mathit \gamma}}$
$53.5$ $\pm4.9$ $\pm2.1$ 2
AAD
2020BA
 ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit Z}}$ ${{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ )
$61.1$ $\pm6.0$ $\pm3.7$ 3
SIRUNYAN
2019BA
 CMS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit Z}}$ ${{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ )
• • We do not use the following data for averages, fits, limits, etc. • •
$57.0$ ${}^{+6.0}_{-5.9}$ ${}^{+4.0}_{-3.3}$ 4
AABOUD
2018CG
 ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit \gamma}}{{\mathit \gamma}}$ , ${{\mathit Z}}$ ${{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ )
$47.9$ ${}^{+9.1}_{-8.6}$ 4
AABOUD
2018CG
 ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit \gamma}}{{\mathit \gamma}}$
$68$ ${}^{+11}_{-10}$ 4
AABOUD
2018CG
 ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit Z}}$ ${{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ )
$69$ ${}^{+10}_{-9}$ $\pm5$ 5
AABOUD
2017CO
 ATLS ${{\mathit p}}{{\mathit p}}$ , 13 TeV, ${{\mathit Z}}$ ${{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$
1  AAD 2022N use 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The quoted value is given for ${\mathit m}_{{{\mathit H}}}$ = 125.09 GeV.
2  AAD 2020BA use 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ where ${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ . The quoted value is given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV and assumes the Standard Model branching ratio.
3  SIRUNYAN 2019BA use 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV.
4  AABOUD 2018CG use 36.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV.
5  AABOUD 2017CO use 36.1 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV with ${{\mathit H}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit Z}^{*}}$ $\rightarrow$ 4 ${{\mathit \ell}}$ where ${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$ for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV. Differential cross sections for the Higgs boson transverse momentum, Higgs boson rapidity, and other related quantities are measured as shown in their Figs. 8 and 9.
References:
AAD 2022N
JHEP 2208 027 Measurements of the Higgs boson inclusive and differential fiducial cross-sections in the diphoton decay channel with pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector
AAD 2020BA
EPJ C80 942 Measurements of the Higgs boson inclusive and differential fiducial cross sections in the 4$\ell$ decay channel at $\sqrt{s}$ = 13 TeV
SIRUNYAN 2019BA
PL B792 369 Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s} =$ 13 TeV
AABOUD 2018CG
PL B786 114 Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector
AABOUD 2017CO
JHEP 1710 132 Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector