${{\mathit \Delta}}$ 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:
B033

${{\mathit \Delta}{(1232)}}$

$I(J^P)$ = $3/2(3/2^{+})$ 
Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).
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▸  ${{\mathit \Delta}{(1232)}}$ POLE POSITIONS
▸  ${{\mathit \Delta}{(1232)}}$ ELASTIC POLE RESIDUES
▸  ${{\mathit \Delta}{(1232)}}$ BREIT-WIGNER MASSES
${\mathit m}_{{{\mathit \Delta}^{0}}}-{\mathit m}_{{{\mathit \Delta}^{++}}}$
 
▸  ${{\mathit \Delta}{(1232)}}$ BREIT-WIGNER WIDTHS
${{\mathit \Delta}^{0}}-{{\mathit \Delta}^{++}}$ WIDTH DIFFERENCE
 
▸  ${{\mathit \Delta}{(1232)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
▸  ${{\mathit \Delta}{(1232)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES
▸  ${{\mathit \Delta}{(1232)}}$ MAGNETIC MOMENTS
The following branching fractions are our estimates, not fits or averages.
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $\text{99.4}$ $\%$ 229
 
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \gamma}}$ $(0.55 - 0.65) \%$ 259
 
$\Gamma_{3}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=1/2 $(0.11 - 0.13) \%$ 259
 
$\Gamma_{4}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=3/2 $(0.44 - 0.52) \%$ 259
 
$\Gamma_{5}$ ${{\mathit p}}{{\mathit e}^{+}}{{\mathit e}^{-}}$ ($4.2$ $\pm0.7$) $ \times 10^{-5}$ 259