pdgLive Home   >   Baryon Summary Table   >   ${{\mathit \Delta}{(1910)}}$   >   Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(1910)}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit K}}$

${{\mathit \Delta}{(1910)}}$ INELASTIC POLE RESIDUE

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

Normalized residue in ${{\mathit N}}$ ${{\mathit \pi}}$ $\rightarrow$ ${{\mathit \Delta}{(1910)}}$ $\rightarrow$ ${{\mathit \Sigma}}{{\mathit K}}$

INSPIRE   PDGID:

B012RS1

MODULUS PHASE ($^\circ{}$) DOCUMENT ID TECN  COMMENT $ 0.002 \pm0.002 $ $138 \pm10$ ROENCHEN 2022 DPWA Multichannel $ 0.07 \pm0.02 $ $-110 \pm30$ ANISOVICH 2012 A DPWA Multichannel • • We do not use the following data for averages, fits, limits, etc. • • $ 0.019 $ $-123$ ROENCHEN 2015 A 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 ANISOVICH 2012A EPJ A48 15 Properties of Baryon Resonances from a Multichannel Partial Wave Analysis

Except where otherwise noted, content of the 2023 Review of Particle Physics is licensed under a Creative Commons Attribution-NonCommercial 4.0 International (CC BY-NC 4.0) license. The publication of the Review of Particle Physics is supported by US DOE, MEXT (Japan), INFN (Italy), JPS and CERN. Individual collaborators receive support for their PDG activities from their respective institutes or funding agencies. © 2023. See LBNL disclaimers.