${{\boldsymbol N}}$ 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

${{\boldsymbol N}{(2060)}}$ $I(J^P)$ = $1/2(5/2^{-})$

Before our 2012 $\mathit Review$, this state appeared in our Listings as the ${{\mathit N}{(2200)}}$.
${{\boldsymbol N}{(2060)}}$ POLE POSITION
REAL PART   $2020\text{ to }2130\text{ }(\approx2070) $ MeV 
$-2{\times }$IMAGINARY PART   $350\text{ to }430\text{ }(\approx400) $ MeV 
${{\boldsymbol N}{(2060)}}$ ELASTIC POLE RESIDUE
MODULUS $\vert \mathit r\vert $   $15\text{ to }30\text{ }(\approx20) $ MeV 
PHASE $\theta $   $-130\text{ to }-90\text{ }(\approx-110) $ $^\circ{}$ 
${{\boldsymbol N}{(2060)}}$ INELASTIC POLE RESIDUE
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \eta}}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit K}}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit N}}{{\mathit \sigma}}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$
Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$
${{\mathit N}{(2060)}}$ BREIT-WIGNER MASS   $2030\text{ to }2200\text{ }(\approx2100) $ MeV 
${{\mathit N}{(2060)}}$ BREIT-WIGNER WIDTH   $300\text{ to }450\text{ }(\approx400) $ MeV 
${{\boldsymbol N}{(2060)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$
${{\boldsymbol N}{(2060)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES
${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$
${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-1/2 amplitude A$_{1/2}$
${{\mathit N}{(2060)}}$ $\rightarrow$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity-3/2 amplitude A$_{3/2}$
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $7 - 12\%$834
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \eta}}$ $2 - 6\%$729
$\Gamma_{3}$ ${{\mathit N}}{{\mathit \omega}}$ $1 - 7\%$600
$\Gamma_{4}$ ${{\mathit \Lambda}}{{\mathit K}}$ seen644
$\Gamma_{5}$ ${{\mathit \Sigma}}{{\mathit K}}$ $1 - 5\%$593
$\Gamma_{6}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ $7 - 19\%$814
$\Gamma_{7}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ 680
$\Gamma_{8}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$ $4 - 10\%$680
$\Gamma_{9}$ ${{\mathit N}}{{\mathit \rho}}$ 605
$\Gamma_{10}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=1/2, ${\mathit P}{\mathrm -wave}$ seen605
$\Gamma_{11}$ ${{\mathit \Lambda}}{{\mathit K}^{*}{(892)}}$ $0.3 - 1.3\%$307
$\Gamma_{12}$ ${{\mathit N}}{{\mathit \sigma}}$ $3 - 9\%$
$\Gamma_{13}$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$ $4 - 14\%$544
$\Gamma_{14}$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ $9 - 21\%$490
$\Gamma_{15}$ ${{\mathit N}{(1680)}}{{\mathit \pi}}$ , ${\mathit S}{\mathrm -wave}$ $8 - 22\%$353
$\Gamma_{16}$ ${{\mathit p}}{{\mathit \gamma}}$ $0.03 - 0.19\%$840
$\Gamma_{17}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=1/2 $0.02 - 0.08\%$840
$\Gamma_{18}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=3/2 $0.01 - 0.10\%$840
$\Gamma_{19}$ ${{\mathit n}}{{\mathit \gamma}}$ $0.003 - 0.07\%$840
$\Gamma_{20}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=1/2 $0.001 - 0.02\%$840
$\Gamma_{21}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=3/2 $0.002 - 0.05\%$840