${{\mathit \Delta}}$ 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:
B010

${{\mathit \Delta}{(1700)}}$

$I(J^P)$ = $3/2(3/2^{-})$ 
Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).
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▸  ${{\mathit \Delta}{(1700)}}$ POLE POSITION
▸  ${{\mathit \Delta}{(1700)}}$ ELASTIC POLE RESIDUE
▸  ${{\mathit \Delta}{(1700)}}$ INELASTIC POLE RESIDUE
${{\mathit \Delta}{(1700)}}$ BREIT-WIGNER MASS 1690 TO 1730 $(\approx 1710 )$ MeV 
 
${{\mathit \Delta}{(1700)}}$ BREIT-WIGNER WIDTH 220 TO 380 $(\approx 300 )$ MeV 
 
▸  ${{\mathit \Delta}{(1700)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
▸  ${{\mathit \Delta}{(1700)}}$ 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)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(10-20) \%$ 588
 
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ >31 $\%$ 557
 
$\Gamma_{3}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ $(9-70) \%$ 394
 
$\Gamma_{4}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit S}{\mathrm -wave}$ $(5 - 54) \%$ 394
 
$\Gamma_{5}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$ $(4 - 16) \%$ 394
 
$\Gamma_{6}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=3/2, ${\mathit S}{\mathrm -wave}$ $(22 - 32) \%$ -1
 
$\Gamma_{7}$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ $(1 - 5) \%$ 133
 
$\Gamma_{8}$ ${{\mathit N}{(1535)}}{{\mathit \pi}}$ $(0.5 - 1.5) \%$ 113
 
$\Gamma_{9}$ ${{\mathit \Delta}{(1232)}}{{\mathit \eta}}$ $(3 - 7) \%$ -1
 
$\Gamma_{10}$ ${{\mathit N}}{{\mathit \gamma}}$ $(0.22 - 0.60) \%$ 598
 
$\Gamma_{11}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=1/2 $(0.12 - 0.30) \%$ 598
 
$\Gamma_{12}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=3/2 $(0.10 - 0.30) \%$ 598