${{\mathit N}}$ 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:
B005

${{\mathit N}{(2060)}}$

$I(J^P)$ = $1/2(5/2^{-})$ 

was ${{\mathit N}{(2200)}}$
Before our 2012 $\mathit Review$, this state appeared in our Listings as the ${{\mathit N}{(2200)}}$.
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▸  ${{\mathit N}{(2060)}}$ POLE POSITION
▸  ${{\mathit N}{(2060)}}$ ELASTIC POLE RESIDUE
▸  ${{\mathit N}{(2060)}}$ INELASTIC POLE RESIDUE
${{\mathit N}{(2060)}}$ BREIT-WIGNER MASS 2030 TO 2200 $(\approx 2100 )$ MeV 
 
${{\mathit N}{(2060)}}$ BREIT-WIGNER WIDTH 300 TO 450 $(\approx 400 )$ MeV 
 
▸  ${{\mathit N}{(2060)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
▸  ${{\mathit N}{(2060)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(7 - 12) \%$ 834
 
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \eta}}$ $(2 - 38) \%$ 729
 
$\Gamma_{3}$ ${{\mathit N}}{{\mathit \omega}}$ $(1 - 7) \%$ 600
 
$\Gamma_{4}$ ${{\mathit \Lambda}}{{\mathit K}}$ $(10 - 20) \%$ 644
 
$\Gamma_{5}$ ${{\mathit \Sigma}}{{\mathit K}}$ $(1 - 5) \%$ 593
 
$\Gamma_{6}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ $(12 - 52) \%$ 814
 
$\Gamma_{7}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit D}{\mathrm -wave}$ $(4 - 10) \%$ 680
 
$\Gamma_{8}$ ${{\mathit N}}{{\mathit \rho}}$ $(5 - 33) \%$ 605
 
$\Gamma_{9}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=1/2, ${\mathit P}{\mathrm -wave}$ <10 $\%$ 605
 
$\Gamma_{10}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=3/2 , ${\mathit D}{\mathrm -wave}$ $(5 - 23) \%$ 605
 
$\Gamma_{11}$ ${{\mathit N}}{{\mathit \sigma}}$ $(3 - 9) \%$  
 
$\Gamma_{12}$ ${{\mathit N}{(1440)}}{{\mathit \pi}}$ $(4 - 14) \%$ 544
 
$\Gamma_{13}$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ $(9 - 21) \%$ 490
 
$\Gamma_{14}$ ${{\mathit N}{(1680)}}{{\mathit \pi}}$ , ${\mathit S}{\mathrm -wave}$ $(8 - 22) \%$ 353
 
$\Gamma_{15}$ ${{\mathit \Lambda}}{{\mathit K}^{*}{(892)}}$ $(0.3 - 1.3) \%$ 307
 
$\Gamma_{16}$ ${{\mathit p}}{{\mathit \gamma}}$ $(0.03 - 0.19) \%$ 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