${{\mathit N}{(1720)}}$ POLE POSITION
B015IM |
$\bf{
150\text{ to }300\text{ }(\approx200) }$
|
OUR ESTIMATE
|
$185$ $\pm6$ |
|
|
DPWA |
$430$ $\pm100$ |
|
|
DPWA |
$184$ $\pm8$ $\pm1$ |
1 |
|
L+P |
$120$ $\pm40$ |
|
|
IPWA |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
$100$ |
|
|
DPWA |
$219$ |
|
|
DPWA |
$118$ |
|
|
DPWA |
$450$ $\pm100$ |
|
|
DPWA |
$233$ $\pm23$ |
|
|
DPWA |
$355$ |
|
|
DPWA |
$94$ |
|
|
DPWA |
$187$ |
|
|
SPED |
1
Fit to the amplitudes of HOEHLER 1979.
|
|
References: |
|
EPJ A58 229
|
Light baryon resonances from a coupled-channel study including $\mathbf{K\Sigma}$ photoproduction |
|
PR C99 055205
|
Updated determination of $N^*$ resonance parameters using a unitary, multichannel formalism |
|
EPJ A51 70
|
${{\mathit \eta}}$ Photoproduction in a Combined Analysis of Pion- and Photon-Induced Reactions |
|
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 C87 015201
|
Eta-meson Production in the Resonance Energy Region |
|
EPJ A48 15
|
Properties of Baryon Resonances from a Multichannel Partial Wave Analysis |
|
PR C82 038203
|
Poles of the Zagreb Analysis Partial-Wave $\mathit T$ Matrices |
|
PR C74 045205
|
Extended Partial-Wave Analysis of ${{\mathit \pi}}{{\mathit N}}$ Scattering Data |
|
PRPL 328 181
|
Baryon Resonance Extraction from ${{\mathit \pi}}$ N Data using a Unitary Multichannel Model |
|
${{\mathit \pi}}{{\mathit N}}$ Newsletter 9 1
|
Determination of ${{\mathit \pi}}{{\mathit N}}$ Resonance Pole Parameters |
|
Toronto Conf. 19
|
Pion $−$ Nucleon Partial Wave Analysis |
|
PR D20 2839 |
Pion Nucleon Partial Wave Amplitudes |
|