# ${{\mathit \Delta}}$ BARYONS ($\mathit S$ = 0, $\mathit I$ = 3/2)

${{\mathit \Delta}^{++}}$ = ${{\mathit u}}{{\mathit u}}{{\mathit u}}$ , ${{\mathit \Delta}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$, ${{\mathit \Delta}^{0}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$, ${{\mathit \Delta}^{-}}$ = ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$
 ${{\mathit \Delta}{(1232)}}$ $3/2{}^{+}$**** ${{\mathit \Delta}{(1600)}}$ $3/2{}^{+}$*** ${{\mathit \Delta}{(1620)}}$ $1/2{}^{-}$**** ${{\mathit \Delta}{(1700)}}$ $3/2{}^{-}$**** ${{\mathit \Delta}{(1750)}}$ $1/2{}^{+}$* ${{\mathit \Delta}{(1900)}}$ $1/2{}^{-}$** ${{\mathit \Delta}{(1905)}}$ $5/2{}^{+}$**** ${{\mathit \Delta}{(1910)}}$ $1/2{}^{+}$**** ${{\mathit \Delta}{(1920)}}$ $3/2{}^{+}$*** ${{\mathit \Delta}{(1930)}}$ $5/2{}^{-}$*** ${{\mathit \Delta}{(1940)}}$ $3/2{}^{-}$** ${{\mathit \Delta}{(1950)}}$ $7/2{}^{+}$**** ${{\mathit \Delta}{(2000)}}$ $5/2{}^{+}$** ${{\mathit \Delta}{(2150)}}$ $1/2{}^{-}$* ${{\mathit \Delta}{(2200)}}$ $7/2{}^{-}$* ${{\mathit \Delta}{(2300)}}$ $9/2{}^{+}$** ${{\mathit \Delta}{(2350)}}$ $5/2{}^{-}$* ${{\mathit \Delta}{(2390)}}$ $7/2{}^{+}$* ${{\mathit \Delta}{(2400)}}$ $9/2{}^{-}$** ${{\mathit \Delta}{(2420)}}$ $11/2{}^{+}$**** ${{\mathit \Delta}{(2750)}}$ $13/2{}^{-}$** ${{\mathit \Delta}{(2950)}}$ $15/2{}^{+}$** ${{\mathit \Delta}{(\sim3000 \text{ Region})}}$Partial-Wave Analyses