${{\mathit \Delta}}$ 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 search

${{\mathit \Delta}{(1600)}}$ $I(J^P)$ = $3/2(3/2^{+})$

Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).
${{\mathit \Delta}{(1600)}}$ POLE POSITION
REAL PART   $1460\text{ to }1560\text{ }(\approx1510) $ MeV 
$-2{\times }$IMAGINARY PART   $200\text{ to }350\text{ }(\approx275) $ MeV 
${{\mathit \Delta}{(1600)}}$ ELASTIC POLE RESIDUE
MODULUS $\vert \mathit r\vert $   $10\text{ to }40\text{ }(\approx25) $ MeV 
PHASE $\theta $   $150\text{ to }210\text{ }(\approx180) $ $^\circ{}$ 
${{\mathit \Delta}{(1600)}}$ INELASTIC POLE RESIDUE
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(1600)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(1600)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$ , ${\mathit F}{\mathrm -wave}$
${{\mathit \Delta}{(1600)}}$ BREIT-WIGNER MASS   $1500\text{ to }1700\text{ }(\approx1600) $ MeV 
${{\mathit \Delta}{(1600)}}$ BREIT-WIGNER WIDTH   $220\text{ to }420\text{ }(\approx320) $ MeV 
${{\mathit \Delta}{(1600)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
${{\mathit \Delta}{(1600)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
${{\mathit \Delta}{(1600)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$
${{\mathit \Delta}{(1600)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$   $-0.045 \pm0.015$ GeV${}^{−1/2}$ 
${{\mathit \Delta}{(1600)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$   $-0.035 \pm0.015$ GeV${}^{−1/2}$ 
The following branching fractions are our estimates, not fits or averages.
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ 10$-25\%$513
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ 75$-90\%$477
$\Gamma_{3}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ 73$-83\%$303
$\Gamma_{4}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ 72$-82\%$303
$\Gamma_{5}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit F}{\mathrm -wave}$ $<2\%$303
$\Gamma_{6}$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$ 98
$\Gamma_{7}$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ seen98
$\Gamma_{8}$ ${{\mathit N}}{{\mathit \gamma}}$ $0.001 - 0.035\%$525
$\Gamma_{9}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=1/2 $0.0 - 0.02\%$525
$\Gamma_{10}$ ${{\mathit N}}{{\mathit \gamma}}$ , helicity=3/2 $0.001 - 0.015\%$525