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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: B014

${{\mathit N}{(1710)}}$ $I(J^P)$ = $1/2(1/2^{+})$

Older and obsolete values are listed and referenced in the 2014 edition, Chinese Physics C38 070001 (2014).

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▸  exp ${{\mathit N}{(1710)}}$ POLE POSITION

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

$-2{\times }$IMAGINARY PART 80 TO 160 $(\approx 120 )$ MeV

▸  exp ${{\mathit N}{(1710)}}$ ELASTIC POLE RESIDUE

MODULUS $\vert \mathit r\vert $ 4 TO 10 $(\approx 7 )$ MeV

PHASE $\theta $ 120 TO 270 $(\approx 190 )$ $^\circ{}$

▸  exp ${{\mathit N}{(1710)}}$ INELASTIC POLE RESIDUE

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \eta}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit K}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit N}{(1535)}}{{\mathit \pi}}$

${{\mathit N}{(1710)}}$ BREIT-WIGNER MASS 1680 TO 1740 $(\approx 1710 )$ MeV

${{\mathit N}{(1710)}}$ BREIT-WIGNER WIDTH 80 TO 200 $(\approx 140 )$ MeV

▸  exp ${{\mathit N}{(1710)}}$ PHOTON DECAY AMPLITUDES AT THE POLE

${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

▸  exp ${{\mathit N}{(1710)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES

${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1710)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1710)}}$ 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)   $\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(5 - 20) \%$ 588   $\Gamma_{2}$ ${{\mathit N}}{{\mathit \eta}}$ $(10 - 50) \%$ 412   $\Gamma_{3}$ ${{\mathit N}}{{\mathit \omega}}$ $(1 - 5) \%$ -1   $\Gamma_{4}$ ${{\mathit \Lambda}}{{\mathit K}}$ $(5 - 25) \%$ 269   $\Gamma_{5}$ ${{\mathit \Sigma}}{{\mathit K}}$ seen 138   $\Gamma_{6}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ $(14 - 48) \%$ 557   $\Gamma_{7}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ $(3 - 9) \%$ 394   $\Gamma_{8}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=1/2, ${\mathit P}{\mathrm -wave}$ $(11 - 23) \%$ -1   $\Gamma_{9}$ ${{\mathit N}}{{\mathit \sigma}}$ <16 $\%$     $\Gamma_{10}$ ${{\mathit N}{(1535)}}{{\mathit \pi}}$ $(9 - 21) \%$ 113   $\Gamma_{11}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=1/2 $(0.002 - 0.08) \%$ 598   $\Gamma_{12}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=1/2 $(0.0 - 0.02) \%$ 597