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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: B064

${{\mathit N}{(1675)}}$ $I(J^P)$ = $1/2(5/2^{-})$

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

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▸  exp ${{\mathit N}{(1675)}}$ POLE POSITION

REAL PART 1650 TO 1660 $(\approx 1655 )$ MeV

$-2{\times }$IMAGINARY PART 120 TO 150 $(\approx 135 )$ MeV

▸  exp ${{\mathit N}{(1675)}}$ ELASTIC POLE RESIDUE

MODULUS $\vert \mathit r\vert $ 22 TO 32 $(\approx 26 )$ MeV

PHASE $\theta $ -27 TO -17 $(\approx -22 )$ $^\circ{}$

▸  exp ${{\mathit N}{(1675)}}$ INELASTIC POLE RESIDUE

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$, ${\mathit D}{\mathrm -wave}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \eta}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit K}}$

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \sigma}}$

${{\mathit N}{(1675)}}$ BREIT-WIGNER MASS 1665 TO 1680 $(\approx 1675 )$ MeV

${{\mathit N}{(1675)}}$ BREIT-WIGNER WIDTH 130 TO 160 $(\approx 145 )$ MeV

▸  exp ${{\mathit N}{(1675)}}$ PHOTON DECAY AMPLITUDES AT THE POLE

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$

▸  exp ${{\mathit N}{(1675)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$ 0.010 TO 0.025 $(\approx 0.018 )$ GeV${}^{−1/2}$

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$ 0.015 TO 0.030 $(\approx 0.022 )$ GeV${}^{−1/2}$

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$ -0.065 TO -0.055 $(\approx -0.060 )$ GeV${}^{−1/2}$

${{\mathit N}{(1675)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$ -0.095 TO -0.075 $(\approx -0.085 )$ GeV${}^{−1/2}$

${{\mathit N}{(1675)}}$ 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)   $\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(38 - 42) \%$ 564   $\Gamma_{2}$ ${{\mathit N}}{{\mathit \eta}}$ < 1 $\%$ 376   $\Gamma_{3}$ ${{\mathit \Lambda}}{{\mathit K}}$ <0.04 $\%$ 216   $\Gamma_{4}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ $(25 - 45) \%$ 532   $\Gamma_{5}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$ $(23 - 37) \%$ 366   $\Gamma_{6}$ ${{\mathit N}}{{\mathit \rho}}$ $(0.1 - 0.9) \%$ -1   $\Gamma_{7}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=1/2 <0.2 $\%$ -1   $\Gamma_{8}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=3/2 , ${\mathit D}{\mathrm -wave}$ $(0.1 - 0.7) \%$ -1   $\Gamma_{9}$ ${{\mathit N}}{{\mathit \sigma}}$ $(3 - 7) \%$     $\Gamma_{10}$ ${{\mathit p}}{{\mathit \gamma}}$ $(0 - 0.02) \%$ 575   $\Gamma_{11}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=1/2 $(0 - 0.01) \%$ 575   $\Gamma_{12}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=3/2 $(0 - 0.01) \%$ 575   $\Gamma_{13}$ ${{\mathit n}}{{\mathit \gamma}}$ $(0 - 0.15) \%$ 574   $\Gamma_{14}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=1/2 $(0 - 0.05) \%$ 574   $\Gamma_{15}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=3/2 $(0 - 0.10) \%$ 574