<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">π</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">−</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math><i>p</i>→<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">π</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">π</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math><i>n</i>near threshold and chiral symmetry breaking
Аннотация
Total cross sections, angular, and mass distributions for the reaction ${\mathrm{\ensuremath{\pi}}}^{\mathrm{\ensuremath{-}}}$p\ensuremath{\rightarrow}${\mathrm{\ensuremath{\pi}}}^{0}$${\mathrm{\ensuremath{\pi}}}^{0}$n have been measured for ${\mathit{p}}_{\mathrm{\ensuremath{\pi}}}^{\mathrm{\ensuremath{-}}}$(lab)=7--140 MeV/c above threshold. The threshold amplitude was used to determine a value for the chiral-symmetry-breaking parameter, \ensuremath{\xi}, of -0.98\ifmmode\pm\else\textpm\fi{}0.52. The \ensuremath{\pi}\ensuremath{\pi} scattering lengths ${\mathit{a}}_{\mathit{I}}$ for isospin I=0 and 2 are derived from this result, together with a current-algebra sum rule. The results are ${\mathit{a}}_{0}$=(0.207\ifmmode\pm\else\textpm\fi{}0.028)${\mathit{m}}_{\mathrm{\ensuremath{\pi}}}^{\mathrm{\ensuremath{-}}1}$ and ${\mathit{a}}_{2}$=(-0.022\ifmmode\pm\else\textpm\fi{}0.011)${\mathit{m}}_{\mathrm{\ensuremath{\pi}}}^{\mathrm{\ensuremath{-}}1}$. These values are consistent with chiral symmetry broken by the Weinberg \ensuremath{\pi}\ensuremath{\pi} interaction and the effects of the ${\mathit{f}}_{0}$(975) scalar meson.
Перевод пока недоступен