${{\mathit \Delta}}$ 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:
B083

${{\mathit \Delta}{(1950)}}$

$I(J^P)$ = $3/2(7/2^{+})$ 
Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).
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▸  ${{\mathit \Delta}{(1950)}}$ POLE POSITION
▸  ${{\mathit \Delta}{(1950)}}$ ELASTIC POLE RESIDUE
▸  ${{\mathit \Delta}{(1950)}}$ INELASTIC POLE RESIDUE
${{\mathit \Delta}{(1950)}}$ BREIT-WIGNER MASS 1915 TO 1950 $(\approx 1930 )$ MeV 
 
${{\mathit \Delta}{(1950)}}$ BREIT-WIGNER WIDTH 235 TO 335 $(\approx 285 )$ MeV 
 
▸  ${{\mathit \Delta}{(1950)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
▸  ${{\mathit \Delta}{(1950)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES
The following branching fractions are our estimates, not fits or averages.
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(35 - 45) \%$ 729
 
$\Gamma_{2}$ ${{\mathit \Sigma}}{{\mathit K}}$ $(0.3 - 0.5) \%$ 441
 
$\Gamma_{3}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ $(37 - 77) \%$ 706
 
$\Gamma_{4}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit F}{\mathrm -wave}$ $(1 - 9) \%$ 560
 
$\Gamma_{5}$ ${{\mathit N}{(1680)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ $(3 - 9) \%$ 191
 
$\Gamma_{6}$ ${{\mathit \Delta}{(1232)}}{{\mathit \eta}}$ < 0.6 $\%$ 349
 
$\Gamma_{7}$ ${{\mathit N}}{{\mathit \gamma}}$ $(0.06 - 0.14) \%$ 737
 
$\Gamma_{8}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=1/2 $(0.03 - 0.05) \%$ 737
 
$\Gamma_{9}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=3/2 $(0.04 - 0.09) \%$ 737