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

INSPIRE   JSON PDGID: B135

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

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▸  exp ${{\mathit \Delta}{(2200)}}$ POLE POSITION

REAL PART 2050 TO 2150 $(\approx 2100 )$ MeV

$-2{\times }$IMAGINARY PART 260 TO 420 $(\approx 340 )$ MeV

▸  exp ${{\mathit \Delta}{(2200)}}$ ELASTIC POLE RESIDUE

MODULUS $\vert \mathit r\vert $

PHASE $\theta $

▸  exp ${{\mathit \Delta}{(2200)}}$ 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 TO 2250 $(\approx 2200 )$ MeV

${{\mathit \Delta}{(2200)}}$ BREIT-WIGNER WIDTH 200 TO 500 $(\approx 350 )$ MeV

▸  exp ${{\mathit \Delta}{(2200)}}$ 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$_{3/2}$

${{\mathit \Delta}{(2200)}}$ DECAY MODES

Mode   Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/ Conf. Level P(MeV/c)   $\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(2 - 8) \%$ 894   $\Gamma_{2}$ ${{\mathit \Sigma}}{{\mathit K}}$ $(1 - 7) \%$ 672   $\Gamma_{3}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ >45 $\%$ 876   $\Gamma_{4}$ ${{\mathit \Delta}}{{\mathit \pi}}$ >45 $\%$ 747   $\Gamma_{5}$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$ >40 $\%$ 747   $\Gamma_{6}$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit G}{\mathrm -wave}$ $(5 - 25) \%$ 747   $\Gamma_{7}$ ${{\mathit \Delta}}{{\mathit \eta}}$ 614   $\Gamma_{8}$ ${{\mathit \Delta}}{{\mathit \eta}}$ , ${\mathit D}{\mathrm -wave}$ seen 614