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${{\mathit N}}$ 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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▸  exp ${{\mathit N}{(1700)}}$ POLE POSITION

REAL PART 1650 TO 1750 $(\approx 1700 )$ MeV

$-2{\times }$IMAGINARY PART 100 TO 300 $(\approx 200 )$ MeV

▸  exp ${{\mathit N}{(1700)}}$ ELASTIC POLE RESIDUE

MODULUS $\vert \mathit r\vert $ 5 TO 50 $(\approx 10 )$ MeV

PHASE $\theta $ -120 TO 0 $(\approx -90 )$ $^\circ{}$

▸  exp ${{\mathit N}{(1700)}}$ INELASTIC POLE RESIDUE

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$, ${\mathit S}{\mathrm -wave}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$, ${\mathit D}{\mathrm -wave}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \sigma}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$, ${\mathit P}{\mathrm -wave}$

${{\mathit N}{(1700)}}$ BREIT-WIGNER MASS 1650 TO 1800 $(\approx 1720 )$ MeV

${{\mathit N}{(1700)}}$ BREIT-WIGNER WIDTH 100 TO 300 $(\approx 200 )$ MeV

▸  exp ${{\mathit N}{(1700)}}$ PHOTON DECAY AMPLITUDES AT THE POLE

${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$

▸  exp ${{\mathit N}{(1700)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES

${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$

${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1700)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$

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