${{\mathit \Delta}}$ 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:
B084

${{\mathit \Delta}{(2420)}}$

$I(J^P)$ = $3/2(11/2^{+})$ 
Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).
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▸  ${{\mathit \Delta}{(2420)}}$ POLE POSITION
▸  ${{\mathit \Delta}{(2420)}}$ ELASTIC POLE RESIDUE
${{\mathit \Delta}{(2420)}}$ BREIT-WIGNER MASS 2300 TO 2600 $(\approx 2450 )$ MeV 
 
${{\mathit \Delta}{(2420)}}$ BREIT-WIGNER WIDTH 300 TO 700 $(\approx 500 )$ MeV 
 
The following branching fractions are our estimates, not fits or averages.
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(5 - 10) \%$ 1040