${{\mathit H}}$ SIGNAL STRENGTHS IN DIFFERENT CHANNELS

The ${{\mathit H}}$ 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( ${{\mathit H}}$ $\rightarrow$ ${{\mathit x}}{{\mathit x}}$) $/$ ($\sigma $ $\cdot{}$ B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit x}}{{\mathit x}}))_{{\mathrm {SM}}}$, for the specified mass value of ${{\mathit H}}$. For the SM predictions, see DITTMAIER 2011, DITTMAIER 2012, and HEINEMEYER 2013A. Results for fiducial and differential cross sections are also listed below.

${{\mathit c}}{{\overline{\mathit c}}}$ Final State

INSPIRE   PDGID:
S126SCC
VALUE CL% DOCUMENT ID TECN  COMMENT
$\bf{<14}$ 95 1
TUMASYAN
2023AH
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}/{{\mathit Z}}{{\mathit H}}$, 13 TeV
• • We do not use the following data for averages, fits, limits, etc. • •
$9.4$ ${}^{+20.3}_{-19.9}$ 2
TUMASYAN
2023AD
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}/{{\mathit Z}}{{\mathit H}}$ (boosted), 13 TeV
$<47$ 95 2
TUMASYAN
2023AD
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}/{{\mathit Z}}{{\mathit H}}$ (boosted), 13 TeV
$-9$ $\pm10$ $\pm11$ 3, 4
AAD
2022W
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}/{{\mathit Z}}{{\mathit H}}$, 13 TeV
$-9$ $\pm10$ $\pm12$ 3, 5
AAD
2022W
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}/{{\mathit Z}}{{\mathit H}}$, 13 TeV
$<26$ 95 3
AAD
2022W
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit W}}{{\mathit H}}/{{\mathit Z}}{{\mathit H}}$, 13 TeV
$37$ $\pm17$ ${}^{+11}_{-9}$ 6
SIRUNYAN
2020AE
 CMS ${{\mathit p}}{{\mathit p}}$, 13 TeV
$<110$ 95 7
AABOUD
2018M
 ATLS ${{\mathit p}}{{\mathit p}}$, 13 TeV
1  TUMASYAN 2023AH search for ${{\mathit V}}{{\mathit H}}$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$ (${{\mathit V}}$ = ${{\mathit W}}$ , ${{\mathit Z}}$) using 138 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The upper limit on ${\mathit \sigma (}$ ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit H}}{)}\cdot{}$B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$) is 0.94 pb at 95$\%$ CL. See their Fig. 4. The quoted values are given for ${\mathit m}_{{{\mathit H}}}$ = 125.38 GeV.
2  TUMASYAN 2023AD search for Higgs produced with transverse momenta greater than 450 GeV and decaying to ${{\mathit c}}{{\overline{\mathit c}}}$ using 138 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV.
3  AAD 2022W search for ${{\mathit V}}{{\mathit H}}$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$ (${{\mathit V}}$ = ${{\mathit W}}$ , ${{\mathit Z}}$) using 139 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collision data at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The results are given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.
4  The analysis of ${{\mathit V}}{{\mathit H}}$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$ is combined with ${{\mathit V}}{{\mathit H}}$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ (AAD 2021AB). The ratio $\vert {{\mathit \kappa}_{{{c}}}}/{{\mathit \kappa}_{{{b}}}}\vert $ is constrained to be less than 4.5 at 95$\%$ CL. See their Fig. 7.
5  The constraint on the charm Yukawa coupling modifier ${{\mathit \kappa}_{{{c}}}}$ is measured to be $\vert {{\mathit \kappa}_{{{c}}}}\vert $ $<$8.5 at 95$\%$ CL. See their Fig. 4.
6  SIRUNYAN 2020AE use 35.9 fb${}^{-1}$ at of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The measured best fit value of ${\mathit \sigma (}$ ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit H}}{)}\cdot{}$B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$) is $2.40$ ${}^{+1.12}_{-1.11}{}^{+0.65}_{-0.61}$ pb (equivalent to $<$ 4.5 pb at 95$\%$ CL upper limit, i.e. 70 times the standard model), where ${{\mathit V}}$ is ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$, ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$, or ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \nu}}{{\mathit \nu}}$ (${{\mathit \ell}}$ = ${{\mathit e}}$ , ${{\mathit \mu}}$). The quoted values are given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.
7  AABOUD 2018M use 36.1 fb${}^{-1}$ at of ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 13 TeV. The upper limit on ${\mathit \sigma (}$ ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit H}}{)}\cdot{}$B( ${{\mathit H}}$ $\rightarrow$ ${{\mathit c}}{{\overline{\mathit c}}}$) is 2.7 pb at 95$\%$ CL. This corresponds to 110 times the standard model. The quoted values are given for ${\mathit m}_{{{\mathit H}}}$ = 125 GeV.
References