${{\boldsymbol N}}$ BARYONS($\boldsymbol S$ = 0, $\boldsymbol I$ = 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 search

# ${{\boldsymbol N}{(1860)}}$ $I(J^P)$ = $1/2(5/2^{+})$

Before the 2012 $\mathit Review$, all the evidence for a $\mathit J{}^{P} = 5/2{}^{+}$ state with a mass above 1800 MeV was filed under a two-star ${{\mathit N}{(2000)}}$. There is now some evidence from ANISOVICH 2012A for two ${}^{}5/2{}^{+}$ states in this region, so we have split the older data (according to mass) between two two-star ${}^{}5/2{}^{+}$ states, an ${{\mathit N}{(1860)}}$ and an ${{\mathit N}{(2000)}}$.
${{\boldsymbol N}{(1860)}}$ POLE POSITION
 REAL PART
 $-2{\times }$IMAGINARY PART
${{\boldsymbol N}{(1860)}}$ ELASTIC POLE RESIDUE
 MODULUS $\vert \mathit r\vert$
 PHASE $\theta$
 ${{\mathit N}{(1860)}}$ BREIT-WIGNER MASS
 ${{\mathit N}{(1860)}}$ BREIT-WIGNER WIDTH
${{\boldsymbol N}{(1860)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES
 ${{\mathit N}{(1860)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
 ${{\mathit N}{(1860)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$
 ${{\mathit N}{(1860)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
 ${{\mathit N}{(1860)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$