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${{\mathit N}{(2120)}}$ POLE POSITION

$-2{\times }$IMAGINARY PART

INSPIRE   PDGID:

B024IM

VALUE (MeV) DOCUMENT ID TECN  COMMENT $\bf{ 200\text{ to }360\text{ }(\approx280) }$ OUR ESTIMATE $345$ $\pm35$ SOKHOYAN 2015 A DPWA Multichannel $296$ $\pm15$ $\pm4$ SVARC 2014 L+P ${{\mathit \pi}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit N}}$ $200$ $\pm80$ CUTKOSKY 1980 IPWA ${{\mathit \pi}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit N}}$ (higher $\mathit m$) • • We do not use the following data for averages, fits, limits, etc. • • $503$ HUNT 2019 DPWA Multichannel $345$ $\pm35$ GUTZ 2014 DPWA Multichannel $340$ $\pm45$ ANISOVICH 2012 A DPWA Multichannel

References:

HUNT 2019 PR C99 055205 Updated determination of $N^*$ resonance parameters using a unitary, multichannel formalism SOKHOYAN 2015A EPJ A51 95 High-Statistics Study of the Reaction ${{\mathit \gamma}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}$2 ${{\mathit \pi}^{0}}$ GUTZ 2014 EPJ A50 74 High Statistics Study of the Reaction SVARC 2014 PR C89 045205 Poles of Karlsruhe-Helsinki KH80 and KA84 Solutions Extracted by using the Laurent-Pietarinen Method ANISOVICH 2012A EPJ A48 15 Properties of Baryon Resonances from a Multichannel Partial Wave Analysis CUTKOSKY 1980 Toronto Conf. 19 Pion $−$ Nucleon Partial Wave Analysis Also PR D20 2839 Pion Nucleon Partial Wave Amplitudes

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