LIGHT UNFLAVORED MESONS ($\mathit S$ = $\mathit C$ = $\mathit B$ = 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 $\mathit I = 0$ (${{\mathit \eta}}$, ${{\mathit \eta}^{\,'}}$, ${{\mathit h}}$, ${{\mathit h}^{\,'}}$, ${{\mathit \omega}}$, ${{\mathit \phi}}$, ${{\mathit f}}$, ${{\mathit f}^{\,'}}$): ${\mathit {\mathit c}}_{{\mathrm {1}}}$( ${{\mathit u}}{{\overline{\mathit u}}}$ $+$ ${{\mathit d}}{{\overline{\mathit d}}}$ ) $+$ ${\mathit {\mathit c}}_{{\mathrm {2}}}$( ${{\mathit s}}{{\overline{\mathit s}}}$ )
Reviews:
Form Factors for Radiative Pion and Kaon Decays (rev.)
Note on Scalar Mesons below 2 GeV (rev.)
The ${{\mathit \rho}{(770)}}$
The Pseudoscalar and Pseudovector Mesons in the 1400 MeV Region (rev.)
The ${{\mathit \rho}{(1450)}}$ and ${{\mathit \rho}{(1700)}}$
${{\mathit \pi}^{\pm}}$
${{\mathit \pi}^{0}}$
${{\mathit \eta}}$
${{\mathit f}_{{0}}{(500)}}~$or ${{\mathit \sigma}}~$was ${{\mathit f}_{{0}}{(600)}}$
${{\mathit \rho}{(770)}}$
${{\mathit \omega}{(782)}}$
${{\mathit \eta}^{\,'}{(958)}}$
${{\mathit f}_{{0}}{(980)}}$
${{\mathit a}_{{0}}{(980)}}$
${{\mathit \phi}{(1020)}}$
${{\mathit h}_{{1}}{(1170)}}$
${{\mathit b}_{{1}}{(1235)}}$
${{\mathit a}_{{1}}{(1260)}}$
${{\mathit f}_{{2}}{(1270)}}$
${{\mathit f}_{{1}}{(1285)}}$
${{\mathit \eta}{(1295)}}$
${{\mathit \pi}{(1300)}}$
${{\mathit a}_{{2}}{(1320)}}$
${{\mathit f}_{{0}}{(1370)}}$
${{\mathit h}_{{1}}{(1380)}}$
${{\mathit \pi}_{{1}}{(1400)}}$
${{\mathit \eta}{(1405)}}$
${{\mathit f}_{{1}}{(1420)}}$
${{\mathit \omega}{(1420)}}$
${{\mathit f}_{{2}}{(1430)}}$
${{\mathit a}_{{0}}{(1450)}}$
${{\mathit \rho}{(1450)}}$
${{\mathit \eta}{(1475)}}$
${{\mathit f}_{{0}}{(1500)}}$
${{\mathit f}_{{1}}{(1510)}}$
${{\mathit f}_{{2}}^{\,'}{(1525)}}$
${{\mathit f}_{{2}}{(1565)}}$
${{\mathit \rho}{(1570)}}$
${{\mathit h}_{{1}}{(1595)}}$
${{\mathit \pi}_{{1}}{(1600)}}$
${{\mathit a}_{{1}}{(1640)}}$
${{\mathit f}_{{2}}{(1640)}}$
${{\mathit \eta}_{{2}}{(1645)}}$
${{\mathit \omega}{(1650)}}$
${{\mathit \omega}_{{3}}{(1670)}}$
${{\mathit \pi}_{{2}}{(1670)}}$
${{\mathit \phi}{(1680)}}$
${{\mathit \rho}_{{3}}{(1690)}}$
${{\mathit \rho}{(1700)}}$
${{\mathit a}_{{2}}{(1700)}}$
${{\mathit f}_{{0}}{(1710)}}$
${{\mathit \eta}{(1760)}}$
${{\mathit \pi}{(1800)}}$
${{\mathit f}_{{2}}{(1810)}}$
${{\mathit X}{(1835)}}$
${{\mathit X}{(1840)}}$
${{\mathit a}_{{1}}{(1420)}}$
${{\mathit \phi}_{{3}}{(1850)}}$
${{\mathit \eta}_{{2}}{(1870)}}$
${{\mathit \pi}_{{2}}{(1880)}}$
${{\mathit \rho}{(1900)}}$
${{\mathit f}_{{2}}{(1910)}}$
${{\mathit a}_{{0}}{(1950)}}$
${{\mathit f}_{{2}}{(1950)}}$
${{\mathit \rho}_{{3}}{(1990)}}$
${{\mathit f}_{{2}}{(2010)}}$
${{\mathit f}_{{0}}{(2020)}}$
${{\mathit a}_{{4}}{(2040)}}$
${{\mathit f}_{{4}}{(2050)}}$
${{\mathit \pi}_{{2}}{(2100)}}$
${{\mathit f}_{{0}}{(2100)}}$
${{\mathit f}_{{2}}{(2150)}}$
${{\mathit \rho}{(2150)}}$
${{\mathit \phi}{(2170)}}$
${{\mathit f}_{{0}}{(2200)}}$
${{\mathit f}_{{J}}{(2220)}}$
${{\mathit \eta}{(2225)}}$
${{\mathit \rho}_{{3}}{(2250)}}$
${{\mathit f}_{{2}}{(2300)}}$
${{\mathit f}_{{4}}{(2300)}}$
${{\mathit f}_{{0}}{(2330)}}$
${{\mathit f}_{{2}}{(2340)}}$
${{\mathit \rho}_{{5}}{(2350)}}$
${{\mathit a}_{{6}}{(2450)}}$
${{\mathit f}_{{6}}{(2510)}}$