${{\mathit N}{(1650)}}$ INELASTIC POLE RESIDUE

The “normalized residue” is the residue divided by $\Gamma _{pole}$/2.

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit N}{(1650)}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}}$ INSPIRE search

B066RS2
MODULUS PHASE ($^\circ{}$) DOCUMENT ID TECN  COMMENT
$ 0.26 \pm0.05 $ $-40 \pm23$
ROENCHEN
2022
DPWA Multichannel
$ 0.26 \pm0.10 $ $110 \pm20$
ANISOVICH
2017A
 DPWA Multichannel
$ 0.10 \pm0.10 $ $95 \pm33$ 1
ANISOVICH
2017A
 L+P ${{\mathit \gamma}}{{\mathit p}}$, ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}}{{\mathit \Lambda}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$ 0.20 $ $-54$
ROENCHEN
2015A
 DPWA Multichannel
$ 0.23 \pm0.09 $ $85 \pm9$
ANISOVICH
2012A
 DPWA Multichannel
1  Statistical error only.
  References:
ROENCHEN 2022
EPJ A58 229 Light baryon resonances from a coupled-channel study including $\mathbf{K\Sigma}$ photoproduction
ANISOVICH 2017A
PRL 119 062004 Strong Evidence for Nucleon Resonances near 1900 MeV
ROENCHEN 2015A
EPJ A51 70 ${{\mathit \eta}}$ Photoproduction in a Combined Analysis of Pion- and Photon-Induced Reactions
ANISOVICH 2012A
EPJ A48 15 Properties of Baryon Resonances from a Multichannel Partial Wave Analysis