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Dispersion relation constrained partial wave analysis of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>π</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:math>elastic and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>π</mml:mi><mml:mi>N</mml:mi><mml:mo>→</mml:mo><mml:mi>η</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:math>scattering data: The baryon spectrum

R. A. ArndtCenter for Nuclear Studies, Department of Physics, The George Washington University, Washington, D.C. 20052, USAW. J. BriscoeCenter for Nuclear Studies, Department of Physics, The George Washington University, Washington, D.C. 20052, USAI. I. StrakovskyCenter for Nuclear Studies, Department of Physics, The George Washington University, Washington, D.C. 20052, USAR. L. WorkmanCenter for Nuclear Studies, Department of Physics, The George Washington University, Washington, D.C. 20052, USAM. M. PavanCenter for Nuclear Studies, Department of Physics, The George Washington University, Washington, D.C. 20052, USA
2004lv
ABI

Аннотация

We present results from a comprehensive partial-wave analysis of ${\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}p$ elastic scattering and charge-exchange data, covering the region from threshold to $2.1\phantom{\rule{0.3em}{0ex}}\text{GeV}$ in the lab pion kinetic energy, employing a coupled-channel formalism to simultaneously fit ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\eta}n$ data to $0.8\phantom{\rule{0.3em}{0ex}}\text{GeV}$. Our main result, solution FA02, utilizes a complete set of forward and fixed-$t$ dispersion relation constraints, from threshold to $1\phantom{\rule{0.3em}{0ex}}\text{GeV}$, and from $t=0$ to $\ensuremath{-}0.4\phantom{\rule{0.3em}{0ex}}{(\text{GeV}∕c)}^{2}$, applied to the $\ensuremath{\pi}N$ elastic amplitude. A large number of systematic checks have been performed, including fits with no charge-exchange data and other database changes, fits with few or no dispersion relation constraints, and changes to the Coulomb correction scheme. We have also reexamined methods used to extract Breit-Wigner resonance parameters. The quality of fit to both data and dispersion relation constraints is superior to our earlier work. The results of these analyses are compared with previous solutions in terms of their resonance spectra and preferred values for couplings and low-energy parameters, including the $\ensuremath{\pi}NN$ coupling constant.

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