${{\mathit N}}$ BARYONS
($\mathit S$ = 0, $\mathit I$ = 1/2)
${{\mathit p}}$, ${{\mathit N}^{+}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$; ${{\mathit n}}$, ${{\mathit N}^{0}}$ = ${\mathit {\mathit u}}$ ${\mathit {\mathit d}}$ ${\mathit {\mathit d}}$
INSPIRE   JSON PDGID:
B018

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

$I(J^P)$ = $1/2(3/2^{-})$ 
Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).
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▸  ${{\mathit N}{(1700)}}$ POLE POSITION
▸  ${{\mathit N}{(1700)}}$ ELASTIC POLE RESIDUE
▸  ${{\mathit N}{(1700)}}$ INELASTIC POLE RESIDUE
${{\mathit N}{(1700)}}$ BREIT-WIGNER MASS 1650 TO 1800 $(\approx 1720 )$ MeV 
 
${{\mathit N}{(1700)}}$ BREIT-WIGNER WIDTH 100 TO 300 $(\approx 200 )$ MeV 
 
▸  ${{\mathit N}{(1700)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
▸  ${{\mathit N}{(1700)}}$ 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)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(7 - 17) \%$ 594
 
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \eta}}$ $(1 - 2) \%$ 422
 
$\Gamma_{3}$ ${{\mathit N}}{{\mathit \omega}}$ $(10 - 34) \%$ -1
 
$\Gamma_{4}$ ${{\mathit \Lambda}}{{\mathit K}}$ $(1 - 2) \%$ 283
 
$\Gamma_{5}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ >89 $\%$ 564
 
$\Gamma_{6}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ $(55 - 85) \%$ 402
 
$\Gamma_{7}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit S}{\mathrm -wave}$ $(50 - 80) \%$ 402
 
$\Gamma_{8}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$ $(4 - 14) \%$ 402
 
$\Gamma_{9}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=3/2, ${\mathit S}{\mathrm -wave}$ $(32 - 44) \%$ 75
 
$\Gamma_{10}$ ${{\mathit N}}{{\mathit \sigma}}$ $(2 - 14) \%$  
 
$\Gamma_{11}$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$ $(3 - 11) \%$ 225
 
$\Gamma_{12}$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$ <4 $\%$ 145
 
$\Gamma_{13}$ ${{\mathit p}}{{\mathit \gamma}}$ $(0.01 - 0.05) \%$ 604
 
$\Gamma_{14}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=1/2 $(0.0 - 0.024) \%$ 604
 
$\Gamma_{15}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=3/2 $(0.002 - 0.026) \%$ 604
 
$\Gamma_{16}$ ${{\mathit n}}{{\mathit \gamma}}$ $(0.01 - 0.13) \%$ 603
 
$\Gamma_{17}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=1/2 $(0.0 - 0.09) \%$ 603
 
$\Gamma_{18}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=3/2 $(0.01 - 0.05) \%$ 603