LIGHT UNFLAVORED MESONS($\boldsymbol S$ = $\boldsymbol C$ = $\boldsymbol B$ = 0) For $\mathit I = 1$ (${{\mathit \pi}}$, ${{\mathit b}}$, ${{\mathit \rho}}$, ${{\mathit a}}$): ${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit d}}}$, ( ${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit u}}}−$ ${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit d}}})/\sqrt {2 }$, ${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit u}}}$;for $\mathit I = 0$ (${{\mathit \eta}}$, ${{\mathit \eta}^{\,'}}$, ${{\mathit h}}$, ${{\mathit h}^{\,'}}$, ${{\mathit \omega}}$, ${{\mathit \phi}}$, ${{\mathit f}}$, ${{\mathit f}^{\,'}}$): ${\mathit {\mathit c}}_{{\mathrm {1}}}$( ${{\mathit u}}{{\overline{\mathit u}}}$ $+$ ${{\mathit d}}{{\overline{\mathit d}}}$ ) $+$ ${\mathit {\mathit c}}_{{\mathrm {2}}}$( ${{\mathit s}}{{\overline{\mathit s}}}$ ) INSPIRE search

# ${{\boldsymbol \rho}{(1700)}}$ $I^G(J^{PC})$ = $1^+(1^{- -})$

 See related review: ${{\mathit \rho}{(1450)}}$ and ${{\mathit \rho}{(1700)}}$
${{\boldsymbol \rho}{(1700)}}$ MASS
 ${{\mathit \eta}}{{\mathit \rho}^{0}}$ AND ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ MODES $1720 \pm20$ MeV
 ${{\mathit \eta}}{{\mathit \rho}^{0}}$ MODE
 ${{\mathit \pi}}{{\mathit \pi}}$ MODE
 ${{\mathit \pi}}{{\mathit \omega}}$ MODE
 ${{\mathit K}}{{\overline{\mathit K}}}$ MODE
 2 ( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ) MODE
 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ MODE
 3( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ) AND 2( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ ) MODES
 ${\mathit m}_{{{\mathit \rho}{(1700)}^{0}}}$ $−$ ${\mathit m}_{{{\mathit \rho}{(1700)}^{\pm}}}$
${{\boldsymbol \rho}{(1700)}}$ WIDTH
 ${{\mathit \eta}}{{\mathit \rho}^{0}}$ AND ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ MODES $250 \pm100$ MeV
 ${{\mathit \eta}}{{\mathit \rho}^{0}}$ MODE
 ${{\mathit \pi}}{{\mathit \pi}}$ MODE
 ${{\mathit K}}{{\overline{\mathit K}}}$ MODE
 2 ( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ) MODE
 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ MODE
 ${{\mathit \omega}}{{\mathit \pi}^{0}}$ MODE
 3( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ) AND 2( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ ) MODES
 ${\Gamma}_{{\mathit \rho}{(1700)}^{0}}$ $−$ ${\Gamma}_{{\mathit \rho}{(1700)}^{\pm}}$