${{\mathit \Delta}{(1950)}}$ INELASTIC POLE RESIDUE

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

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(1950)}}$ $\rightarrow$ ${{\mathit \Delta}}{{\mathit \pi}}$, ${\mathit F}{\mathrm -wave}$ INSPIRE search

B083RS2
MODULUS () PHASE ($^\circ{}$) DOCUMENT ID TECN  COMMENT
$ 0.30 \pm0.27 $ $166 \pm1$
ROENCHEN
2022
DPWA Multichannel
$ 0.12 \pm0.04 $ undefined
SOKHOYAN
2015A
 DPWA Multichannel
• • • We do not use the following data for averages, fits, limits, etc. • • •
$ 0.54 $ $131$
ROENCHEN
2015A
 DPWA Multichannel
$ 0.12 \pm0.04 $ $12 \pm10$
ANISOVICH
2012A
 DPWA Multichannel
  References:
ROENCHEN 2022
EPJ A58 229 Light baryon resonances from a coupled-channel study including $\mathbf{K\Sigma}$ photoproduction
ROENCHEN 2015A
EPJ A51 70 ${{\mathit \eta}}$ Photoproduction in a Combined Analysis of Pion- and Photon-Induced Reactions
SOKHOYAN 2015A
EPJ A51 95 High-Statistics Study of the Reaction ${{\mathit \gamma}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}$2 ${{\mathit \pi}^{0}}$
ANISOVICH 2012A
EPJ A48 15 Properties of Baryon Resonances from a Multichannel Partial Wave Analysis