GAUGE AND HIGGS BOSONS INSPIRE search

#### ${{\mathit H}^{0}}$

$J$ = $0$
In the following ${{\mathit H}^{0}}$ 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 ${{\mathit H}^{0}}$ 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.
 ${{\mathit H}^{0}}$ MASS $125.25 \pm0.17$ GeV (S = 1.5)
 ${{\mathit H}^{0}}$ SPIN AND $\mathit CP$ PROPERTIES
 ${{\mathit H}^{0}}$ DECAY WIDTH $3.2 {}^{+2.8}_{-2.2}$ MeV
${{\mathit H}^{0}}$ SIGNAL STRENGTHS IN DIFFERENT CHANNELS
 Combined Final States $1.13 \pm0.06$
 ${{\mathit W}}{{\mathit W}^{*}}$ Final State $1.19 \pm0.12$
 ${{\mathit Z}}{{\mathit Z}^{*}}$ Final State $1.01 \pm0.07$
 ${{\mathit \gamma}}{{\mathit \gamma}}$ Final State $1.10 \pm0.07$
 ${{\mathit c}}{{\overline{\mathit c}}}$ Final State $37 \pm20$
 ${{\mathit b}}{{\overline{\mathit b}}}$ Final State $0.98 \pm0.12$
 ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ Final State $1.19 \pm0.34$
 ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ Final State $1.15 {}^{+0.16}_{-0.15}$
 ${{\mathit Z}}{{\mathit \gamma}}$ Final State $<3.6$   CL=95.0%
 ${{\mathit \gamma}^{*}}{{\mathit \gamma}}$ Final State $1.5 \pm0.5$
Higgs Yukawa couplings
 top Yukawa coupling
OTHER ${{\mathit H}^{0}}$ PRODUCTION PROPERTIES
 ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit H}^{0}}$ Production $1.10 \pm0.18$
 ${{\mathit H}^{0}}{{\mathit H}^{0}}$ Production
 ${{\mathit t}}{{\mathit H}^{0}}$ production $6 \pm4$
 ${{\mathit H}^{0}}$ Production Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV $56 \pm4$ pb
 $\Gamma_{1}$ ${{\mathit W}}{{\mathit W}^{*}}$
 $\Gamma_{2}$ ${{\mathit Z}}{{\mathit Z}^{*}}$
 $\Gamma_{3}$ ${{\mathit \gamma}}{{\mathit \gamma}}$ 62625
 $\Gamma_{4}$ ${{\mathit b}}{{\overline{\mathit b}}}$
 $\Gamma_{5}$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ $<3.6\times 10^{-4}$ CL=95% 62625
 $\Gamma_{6}$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ 62625
 $\Gamma_{7}$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ 62600
 $\Gamma_{8}$ ${{\mathit Z}}{{\mathit \gamma}}$ 29431
 $\Gamma_{9}$ ${{\mathit Z}}{{\mathit \rho}{(770)}}$ $<1.21\%$ CL=95% 29423
 $\Gamma_{10}$ ${{\mathit Z}}{{\mathit \phi}{(1020)}}$ $<3.6\times 10^{-3}$ CL=95% 29417
 $\Gamma_{11}$ ${{\mathit Z}}{{\mathit \eta}_{{c}}}$ 29315
 $\Gamma_{12}$ ${{\mathit Z}}{{\mathit J / \psi}}$ 29306
 $\Gamma_{13}$ ${{\mathit \gamma}^{*}}{{\mathit \gamma}}$ 62625
 $\Gamma_{14}$ ${{\mathit J / \psi}}{{\mathit \gamma}}$ $<3.5\times 10^{-4}$ CL=95% 62587
 $\Gamma_{15}$ ${{\mathit J / \psi}}{{\mathit J / \psi}}$ $<1.8\times 10^{-3}$ CL=95% 62548
 $\Gamma_{16}$ ${{\mathit \psi}{(2S)}}{{\mathit \gamma}}$ $<2.0\times 10^{-3}$ CL=95% 62571
 $\Gamma_{17}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \gamma}}$ $<4.9\times 10^{-4}$ CL=95% 62268
 $\Gamma_{18}$ ${{\mathit \Upsilon}{(2S)}}{{\mathit \gamma}}$ $<5.9\times 10^{-4}$ CL=95% 62224
 $\Gamma_{19}$ ${{\mathit \Upsilon}{(3S)}}{{\mathit \gamma}}$ $<5.7\times 10^{-4}$ CL=95% 62197
 $\Gamma_{20}$ ${{\mathit \Upsilon}{(nS)}}{{\mathit \Upsilon}{(mS)}}$ $<1.4\times 10^{-3}$ CL=95%
 $\Gamma_{21}$ ${{\mathit \rho}{(770)}}{{\mathit \gamma}}$ $<8.8\times 10^{-4}$ CL=95% 62623
 $\Gamma_{22}$ ${{\mathit \phi}{(1020)}}{{\mathit \gamma}}$ $<4.8\times 10^{-4}$ CL=95% 62621
 $\Gamma_{23}$ ${{\mathit e}}{{\mathit \mu}}$ $<6.1\times 10^{-5}$ CL=95% 62625
 $\Gamma_{24}$ ${{\mathit e}}{{\mathit \tau}}$ $<2.2\times 10^{-3}$ CL=95% 62612
 $\Gamma_{25}$ ${{\mathit \mu}}{{\mathit \tau}}$ $<1.5\times 10^{-3}$ CL=95% 62612
 $\Gamma_{26}$ ${\mathrm {invisible}}$ $<19\%$ CL=95%
 $\Gamma_{27}$ ${{\mathit \gamma}}$ ${\mathrm {invisible}}$
 FOOTNOTES