${{\mathit N}{(2100)}}$ POLE POSITION
| B132IM |
| $\bf{
240\text{ to }340\text{ }(\approx300) }$
|
OUR ESTIMATE
|
| $430$ $\pm65$ |
|
|
DPWA |
| $337$ $\pm10$ $\pm4$ |
1 |
|
L+P |
| $240$ $\pm80$ |
|
|
IPWA |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $545$ |
|
|
DPWA |
| $290$ $\pm30$ |
|
|
DPWA |
| $346$ $\pm80$ |
|
|
DPWA |
| $622$ |
|
|
DPWA |
|
1
Fit to the amplitudes of HOEHLER 1979.
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|
| References: |
|
|
PR C112 015202
|
Decays of $N^*$ and $?^*$ resonances into $N?$, $??$, and $N?$ |
|
|
PR C99 055205
|
Updated determination of $N^*$ resonance parameters using a unitary, multichannel formalism |
|
|
EPJ A51 95
|
High-Statistics Study of the Reaction ${{\mathit \gamma}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}$2 ${{\mathit \pi}^{0}}$ |
|
|
PR C89 045205
|
Poles of Karlsruhe-Helsinki KH80 and KA84 Solutions Extracted by using the Laurent-Pietarinen Method |
|
|
PR C82 038203
|
Poles of the Zagreb Analysis Partial-Wave $\mathit T$ Matrices |
|
|
PRPL 328 181
|
Baryon Resonance Extraction from ${{\mathit \pi}}$ N Data using a Unitary Multichannel Model |
|
|
Toronto Conf. 19
|
Pion $−$ Nucleon Partial Wave Analysis |
|
|
PR D20 2839 |
Pion Nucleon Partial Wave Amplitudes |
|