GAUGE AND HIGGS BOSONS
 INSPIRE search

${{\mathit H}}$ $J$ = $0$ 


was ${{\mathit H}^{0}}$
In the following ${{\mathit H}}$ refers to the signal that has been discovered in the Higgs searches. Whereas the observed signal is labeled as a spin 0 particle and is called a Higgs Boson, the detailed properties of ${{\mathit H}}$ and its role in the context of electroweak symmetry breaking need to be further clarified. These issues are addressed by the measurements listed below. Concerning mass limits and cross section limits that have been obtained in the searches for neutral and charged Higgs bosons, see the sections ``Searches for Neutral Higgs Bosons'' and ``Searches for Charged Higgs Bosons (${{\mathit H}^{\pm}}$ and ${{\mathit H}^{\pm\pm}}$)'', respectively.
${{\mathit H}}$ MASS   $125.13 \pm0.11$ GeV (S = 1.5)
${{\mathit H}}$ SPIN AND $\mathit CP$ PROPERTIES
${{\mathit H}}$ DECAY WIDTH   $3.0 {}^{+1.5}_{-0.7}$ MeV 
${{\mathit H}}$ SIGNAL STRENGTHS IN DIFFERENT CHANNELS
Combined final state   $1.03 \pm0.04$  
${{\mathit W}}{{\mathit W}^{*}}$ final state   $1.00 \pm0.08$  
${{\mathit Z}}{{\mathit Z}^{*}}$ final state   $1.02 \pm0.08$  
${{\mathit \gamma}}{{\mathit \gamma}}$ final state   $1.10 \pm0.06$  
${{\mathit c}}{{\overline{\mathit c}}}$ final state   $-0.5 \pm3.4$  
${{\mathit b}}{{\overline{\mathit b}}}$ final state   $0.94 \pm0.11$  
${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ final state   $1.31 \pm0.29$  
${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ final state   $0.91 \pm0.09$  
${{\mathit Z}}{{\mathit \gamma}}$ final state   $2.2 \pm0.7$  
${{\mathit \gamma}^{*}}{{\mathit \gamma}}$ final state   $1.5 \pm0.5$  
HIGGS COUPLINGS
Fermion coupling (${{\mathit \kappa}_{{{F}}}}$)   $0.94 \pm0.05$  
Gauge boson coupling (${{\mathit \kappa}_{{{V}}}}$)   $1.023 \pm0.026$  
${{\mathit W}}$ boson coupling (${{\mathit \kappa}_{{{W}}}}$)
${{\mathit Z}}$ boson coupling (${{\mathit \kappa}_{{{Z}}}}$)
top Yukawa coupling (${{\mathit \kappa}_{{{t}}}}$)
bottom quark Yukawa coupling (${{\mathit \kappa}_{{{b}}}}$)
charm quark Yukawa coupling (${{\mathit \kappa}_{{{c}}}}$)
strange quark Yukawa coupling (${{\mathit \kappa}_{{{s}}}}$)
down quark Yukawa coupling (${{\mathit \kappa}_{{{d}}}}$)
up quark Yukawa coupling (${{\mathit \kappa}_{{{u}}}}$)
tau Yukawa coupling (${{\mathit \kappa}_{{{\tau}}}}$)
muon Yukawa couping (${{\mathit \kappa}_{{{\mu}}}}$)
photon effective coupling (${{\mathit \kappa}_{{{\gamma}}}}$)
gluon effective coupling (${{\mathit \kappa}_{{{gluon}}}}$)
${{\mathit Z}}{{\mathit \gamma}}$ effective coupling (${{\mathit \kappa}}_{{{\mathit Z}}{{\mathit \gamma}}}$)
OTHER ${{\mathit H}}$ PRODUCTION PROPERTIES
${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}}$ production   $0.91 {}^{+0.20}_{-0.18}$  (S = 1.6)
${{\mathit b}}{{\overline{\mathit b}}}{{\mathit H}}$ production   $<3.7$   CL=95.0%
${{\mathit t}}{{\mathit H}}$ production   $7.1 \pm2.5$  
${{\mathit c}}{{\mathit H}}$ production
VBS/VBF ${{\mathit W}}{{\mathit H}}$ production
${{\mathit \gamma}}{{\mathit H}}$ production
${{\mathit H}}{{\mathit H}}$ production   $<2.4$   CL=95.0%
${{\mathit H}}{{\mathit H}}{{\mathit H}}$ production   $<760$   CL=95.0%
Higgs trilinear self coupling modifier ${{\mathit \kappa}_{{{\lambda}}}}$   $3.8 {}^{+2.1}_{-4.0}$  
Higgs quartic self coupling modifier ${{\mathit \kappa}_{{{4}}}}$
Higgs-gauge boson quartic coupling modifier ${{\mathit \kappa}_{{{2V}}}}$   $1.02 \pm0.23$  
${{\mathit H}}$ production cross section in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV   $56.8 \pm3.4$ pb 
${{\mathit H}}$ production cross section in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13.6 TeV   $58 \pm9$ pb 
$\Gamma_{1}$ ${{\mathit W}}{{\mathit W}^{*}}$  $(25.7\pm{2.5})\%$
$\Gamma_{2}$ ${{\mathit Z}}{{\mathit Z}^{*}}$  $(2.80\pm{0.30})\%$
$\Gamma_{3}$ ${{\mathit \gamma}}{{\mathit \gamma}}$  $(2.50\pm{0.20})\times 10^{-3}$ 62565
$\Gamma_{4}$ ${{\mathit b}}{{\overline{\mathit b}}}$  $(53\pm{8})\%$
$\Gamma_{5}$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$  $<3.0\times 10^{-4}$ CL=95%62565
$\Gamma_{6}$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$  $(3.0\pm{0.9})\times 10^{-4}$ 62565
$\Gamma_{7}$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$  $(6.0^{+0.8}_{-0.7})\%$ 62540
$\Gamma_{8}$ ${{\mathit Z}}{{\mathit \gamma}}$  $(3.4\pm{1.1})\times 10^{-3}$ 29339
$\Gamma_{9}$ ${{\mathit Z}}{{\mathit \rho}{(770)}}$  $<1.21\%$ CL=95%29332
$\Gamma_{10}$ ${{\mathit Z}}{{\mathit \phi}{(1020)}}$  $<3.6\times 10^{-3}$ CL=95%29326
$\Gamma_{11}$ ${{\mathit Z}}{{\mathit \eta}_{{{c}}}}$  29223
$\Gamma_{12}$ ${{\mathit Z}}{{\mathit J / \psi}}$  $<1.9\times 10^{-3}$ CL=95%29214
$\Gamma_{13}$ ${{\mathit Z}}{{\mathit \psi}{(2S)}}$  $<6.6\times 10^{-3}$ CL=95%29162
$\Gamma_{14}$ ${{\mathit J / \psi}}{{\mathit \gamma}}$  $<2.0\times 10^{-4}$ CL=95%62527
$\Gamma_{15}$ ${{\mathit J / \psi}}{{\mathit J / \psi}}$  $<3.8\times 10^{-4}$ CL=95%62489
$\Gamma_{16}$ ${{\mathit \psi}{(2S)}}{{\mathit \gamma}}$  $<9.9\times 10^{-4}$ CL=95%62511
$\Gamma_{17}$ ${{\mathit \psi}{(2S)}}{{\mathit J / \psi}}$  $<2.1\times 10^{-3}$ CL=95%62473
$\Gamma_{18}$ ${{\mathit \psi}{(2S)}}{{\mathit \psi}{(2S)}}$  $<3.0\times 10^{-3}$ CL=95%62457
$\Gamma_{19}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \gamma}}$  $<2.5\times 10^{-4}$ CL=95%62208
$\Gamma_{20}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \Upsilon}{(1S)}}$  $<1.7\times 10^{-3}$ CL=95%61846
$\Gamma_{21}$ ${{\mathit \Upsilon}{(2S)}}{{\mathit \gamma}}$  $<4.2\times 10^{-4}$ CL=95%62164
$\Gamma_{22}$ ${{\mathit \Upsilon}{(3S)}}{{\mathit \gamma}}$  $<3.4\times 10^{-4}$ CL=95%62137
$\Gamma_{23}$ ${{\mathit \Upsilon}{(nS)}}{{\mathit \Upsilon}{(mS)}}$  $<3.5\times 10^{-4}$ CL=95%
$\Gamma_{24}$ ${{\mathit D}^{*}}{{\mathit \gamma}}$  $<1.0\times 10^{-3}$ CL=95%62549
$\Gamma_{25}$ ${{\mathit \rho}{(770)}}{{\mathit \gamma}}$  $<3.7\times 10^{-4}$ CL=95%62563
$\Gamma_{26}$ ${{\mathit \omega}{(782)}}{{\mathit \gamma}}$  $<5.5\times 10^{-4}$ CL=95%62563
$\Gamma_{27}$ ${{\mathit K}^{*}{(892)}}{{\mathit \gamma}}$  $<2.2\times 10^{-4}$ CL=95%62562
$\Gamma_{28}$ ${{\mathit \phi}{(1020)}}{{\mathit \gamma}}$  $<3.0\times 10^{-4}$ CL=95%62561
$\Gamma_{29}$ ${{\mathit e}}{{\mathit \mu}}$  $<4.4\times 10^{-5}$ CL=95%62565
$\Gamma_{30}$ ${{\mathit e}}{{\mathit \tau}}$  $<2.0\times 10^{-3}$ CL=95%62553
$\Gamma_{31}$ ${{\mathit \mu}}{{\mathit \tau}}$  $<1.5\times 10^{-3}$ CL=95%62553
$\Gamma_{32}$ ${\mathrm {invisible}}$  $<10.7\%$ CL=95%
$\Gamma_{33}$ ${{\mathit \gamma}}$ ${\mathrm {invisible}}$  $<1.3\%$ CL=95%