${\boldsymbol {\boldsymbol c}}$ ${\boldsymbol {\overline{\boldsymbol c}}}$ MESONS
(including possibly non- ${\boldsymbol {\boldsymbol q}}$ ${\boldsymbol {\overline{\boldsymbol q}}}$ states)
INSPIRE search

${{\boldsymbol \psi}{(4040)}}$ $I^G(J^{PC})$ = $0^-(1^{- -})$

${{\mathit \psi}{(4040)}}$ MASS   $4039 \pm1$ MeV 
${{\mathit \psi}{(4040)}}$ WIDTH   $80 \pm10$ MeV 
Due to the complexity of the ${{\mathit c}}{{\overline{\mathit c}}}$ threshold region, in this listing, ``seen'' (``not seen'') means that a cross section for the mode in question has been measured at effective $\sqrt {s }$ near this particle's central mass value, more (less) than 2${{\mathit \sigma}}$ above zero, without regard to any peaking behavior in $\sqrt {s }$ or absence thereof. See mode listing(s) for details and references.
$\Gamma_{1}$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ $(1.07\pm{0.16})\times 10^{-5}$2019
$\Gamma_{2}$ ${{\mathit D}}{{\overline{\mathit D}}}$ seen775
$\Gamma_{3}$ ${{\mathit D}^{0}}{{\overline{\mathit D}}^{0}}$ seen775
$\Gamma_{4}$ ${{\mathit D}^{+}}{{\mathit D}^{-}}$ seen763
$\Gamma_{5}$ ${{\mathit D}^{*}}{{\overline{\mathit D}}}$ + c.c. seen569
$\Gamma_{6}$ ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{0}}$ + c.c. seen575
$\Gamma_{7}$ ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{-}}$ + c.c. seen561
$\Gamma_{8}$ ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ seen193
$\Gamma_{9}$ ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{*}{(2007)}^{0}}$ seen226
$\Gamma_{10}$ ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{*}{(2010)}^{-}}$ seen193
$\Gamma_{11}$ ${{\mathit D}}{{\overline{\mathit D}}}{{\mathit \pi}}$ (excl. ${{\mathit D}^{*}}{{\overline{\mathit D}}}$ ) 
$\Gamma_{12}$ ${{\mathit D}^{0}}{{\mathit D}^{-}}{{\mathit \pi}^{+}}$ +c.c. (excl. ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{0}}$ +c.c., ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{-}}$ +c.c.) not seen
$\Gamma_{13}$ ${{\mathit D}}{{\overline{\mathit D}}^{*}}{{\mathit \pi}}$ (excl. ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ ) not seen
$\Gamma_{14}$ ${{\mathit D}^{0}}{{\overline{\mathit D}}^{*-}}{{\mathit \pi}^{+}}$ +c.c. (excl. ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{*}{(2010)}^{-}}$ ) seen
$\Gamma_{15}$ ${{\mathit D}_{{s}}^{+}}{{\mathit D}_{{s}}^{-}}$ seen452
$\Gamma_{16}$ ${{\mathit J / \psi}{(1S)}}$ hadrons 
$\Gamma_{17}$ ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<4\times 10^{-3}$CL=90%794
$\Gamma_{18}$ ${{\mathit J / \psi}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ $<2\times 10^{-3}$CL=90%797
$\Gamma_{19}$ ${{\mathit J / \psi}}{{\mathit \eta}}$ $(5.2\pm{0.7})\times 10^{-3}$675
$\Gamma_{20}$ ${{\mathit J / \psi}}{{\mathit \pi}^{0}}$ $<2.8\times 10^{-4}$CL=90%823
$\Gamma_{21}$ ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ $<2\times 10^{-3}$CL=90%746
$\Gamma_{22}$ ${{\mathit \chi}_{{c1}}}{{\mathit \gamma}}$ $<3.4\times 10^{-3}$CL=90%494
$\Gamma_{23}$ ${{\mathit \chi}_{{c2}}}{{\mathit \gamma}}$ $<5\times 10^{-3}$CL=90%454
$\Gamma_{24}$ ${{\mathit \chi}_{{c1}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ $<1.1\%$CL=90%306
$\Gamma_{25}$ ${{\mathit \chi}_{{c2}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ $<3.2\%$CL=90%233
$\Gamma_{26}$ ${{\mathit h}_{{c}}{(1P)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<3\times 10^{-3}$CL=90%403
$\Gamma_{27}$ ${{\mathit \phi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<3\times 10^{-3}$CL=90%1880
$\Gamma_{28}$ ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<2.9\times 10^{-4}$CL=90%1578
$\Gamma_{29}$ ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}{{\mathit \pi}^{0}}$ $<9\times 10^{-5}$CL=90%1636
$\Gamma_{30}$ ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}{{\mathit \eta}}$ $<3.0\times 10^{-4}$CL=90%1452
$\Gamma_{31}$ ${{\mathit \Sigma}^{+}}{{\overline{\mathit \Sigma}}^{-}}$ $<1.3\times 10^{-4}$CL=90%1632
$\Gamma_{32}$ ${{\mathit \Sigma}^{0}}{{\overline{\mathit \Sigma}}^{0}}$ $<7\times 10^{-5}$CL=90%1630
$\Gamma_{33}$ ${{\mathit \Xi}^{+}}{{\overline{\mathit \Xi}}^{-}}$ $<1.6\times 10^{-4}$CL=90%1527
$\Gamma_{34}$ ${{\mathit \Xi}^{0}}{{\overline{\mathit \Xi}}^{0}}$ $<1.8\times 10^{-4}$CL=90%1533
$\Gamma_{35}$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ 2017