${{\mathit N}}$ 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:
B144

${{\mathit N}{(1900)}}$

$I(J^P)$ = $1/2(3/2^{+})$ 
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▸  ${{\mathit N}{(1900)}}$ POLE POSITION
▸  ${{\mathit N}{(1900)}}$ ELASTIC POLE RESIDUE
▸  ${{\mathit N}{(1900)}}$ INELASTIC POLE RESIDUE
${{\mathit N}{(1900)}}$ BREIT-WIGNER MASS 1890 TO 1950 $(\approx 1920 )$ MeV 
 
${{\mathit N}{(1900)}}$ BREIT-WIGNER WIDTH 100 TO 320 $(\approx 200 )$ MeV 
 
▸  ${{\mathit N}{(1900)}}$ PHOTON DECAY AMPLITUDES AT THE POLE
▸  ${{\mathit N}{(1900)}}$ BREIT-WIGNER PHOTON DECAY AMPLITUDES
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit N}}{{\mathit \pi}}$ $(1 - 20) \%$ 723
 
$\Gamma_{2}$ ${{\mathit N}}{{\mathit \eta}}$ $(2 - 14) \%$ 595
 
$\Gamma_{3}$ ${{\mathit N}}{{\mathit \eta}^{\,'}}$ $(4 - 8) \%$ 151
 
$\Gamma_{4}$ ${{\mathit N}}{{\mathit \omega}}$ $(7 - 13) \%$ 424
 
$\Gamma_{5}$ ${{\mathit \Lambda}}{{\mathit K}}$ $(2 - 20) \%$ 495
 
$\Gamma_{6}$ ${{\mathit \Sigma}}{{\mathit K}}$ $(3 - 7) \%$ 431
 
$\Gamma_{7}$ ${{\mathit N}}{{\mathit \pi}}{{\mathit \pi}}$ >56 $\%$ 699
 
$\Gamma_{8}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ $(30 - 70) \%$ 553
 
$\Gamma_{9}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit P}{\mathrm -wave}$ $(9 - 25) \%$ 553
 
$\Gamma_{10}$ ${{\mathit \Delta}{(1232)}}{{\mathit \pi}}$ , ${\mathit F}{\mathrm -wave}$ $(21 - 45) \%$ 553
 
$\Gamma_{11}$ ${{\mathit N}}{{\mathit \rho}}$ , $\mathit S$=1/2 $(25 - 40) \%$ 432
 
$\Gamma_{12}$ ${{\mathit N}}{{\mathit \sigma}}$ $(1 - 7) \%$  
 
$\Gamma_{13}$ ${{\mathit N}{(1520)}}{{\mathit \pi}}$ $(7 - 23) \%$ 341
 
$\Gamma_{14}$ ${{\mathit N}{(1535)}}{{\mathit \pi}}$ $(4 - 10) \%$ 328
 
$\Gamma_{15}$ ${{\mathit \Lambda}}{{\mathit K}^{*}{(892)}}$ < 0.2 $\%$ -1
 
$\Gamma_{16}$ ${{\mathit p}}{{\mathit \gamma}}$ $(0.001 - 0.025) \%$ 731
 
$\Gamma_{17}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=1/2 $(0.001 - 0.021) \%$ 731
 
$\Gamma_{18}$ ${{\mathit p}}{{\mathit \gamma}}$ , helicity=3/2 <0.003 $\%$ 731
 
$\Gamma_{19}$ ${{\mathit n}}{{\mathit \gamma}}$ <0.040 $\%$ 730
 
$\Gamma_{20}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=1/2 <0.007 $\%$ 730
 
$\Gamma_{21}$ ${{\mathit n}}{{\mathit \gamma}}$ , helicity=3/2 <0.033 $\%$ 730