${{\boldsymbol \Delta}}$ BARYONS
($\boldsymbol S$ = 0, $\boldsymbol I$ = 3/2)
${{\mathit \Delta}^{++}}$ = ${{\mathit u}}{{\mathit u}}{{\mathit u}}$ , ${{\mathit \Delta}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$, ${{\mathit \Delta}^{0}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$, ${{\mathit \Delta}^{-}}$ = ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$
INSPIRE search

${{\boldsymbol \Delta}{(2200)}}$ $I(J^P)$ = $3/2(7/2^{-})$ 

${{\boldsymbol \Delta}{(2200)}}$ POLE POSITION
REAL PART   $2050\text{ to }2150\text{ }(\approx2100) $ MeV 
$-2{\times }$IMAGINARY PART   $260\text{ to }420\text{ }(\approx340) $ MeV 
${{\boldsymbol \Delta}{(2200)}}$ ELASTIC POLE RESIDUE
MODULUS $\vert \mathit r\vert $
PHASE $\theta $
${{\boldsymbol \Delta}{(2200)}}$ INELASTIC POLE RESIDUE
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(2200)}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit K}}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(2200)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(2200)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit G}{\mathrm -wave}$
${{\mathit \Delta}{(2200)}}$ BREIT-WIGNER MASS   $2150\text{ to }2250\text{ }(\approx2200) $ MeV 
${{\mathit \Delta}{(2200)}}$ BREIT-WIGNER WIDTH   $200\text{ to }500\text{ }(\approx350) $ MeV 
${{\boldsymbol \Delta}{(2200)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
${{\mathit \Delta}{(2200)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
${{\mathit \Delta}{(2200)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$  $2 - 8\%$ 894
$\Gamma_{2}$ ${{\mathit \Sigma}}{{\mathit K}}$  $1 - 7\%$ 672
$\Gamma_{3}$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$  $40 - 100\%$ 747
$\Gamma_{4}$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit G}{\mathrm -wave}$  $5 - 25\%$ 747
$\Gamma_{5}$ ${{\mathit \Delta}}{{\mathit \eta}}$ , ${\mathit D}{\mathrm -wave}$  seen 614