Strange-Particle Production in π−p Interactions from 1.5 to 4.2 BeVc . II. Two-Body Final States
O. I. Dahl, Lyndon M. Hardy, Richard I. Hess, Janos Kirz, Donald H. Miller, Joseph A. Schwartz
Abstract
O. I. Dahl, Lyndon M. Hardy, Richard I. Hess, Janos Kirz, Donald H. Miller, Joseph A. Schwartz
Abstract
The reactions ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0},{\ensuremath{\Sigma}}^{0}{K}^{0}$, and ${\ensuremath{\Sigma}}^{\ensuremath{-}}{K}^{+}$ in the 1.5- to 4.2-$\frac{\mathrm{BeV}}{c}$ momentum range were studied in the Lawrence Radiation Laboratory's 72-in. hydrogen bubble chamber. The total cross sections for the three reactions decrease as $E_{\mathrm{c}.\mathrm{m}.}^{}{}_{}{}^{\ensuremath{-}3.6}$, $E_{\mathrm{c}.\mathrm{m}.}^{}{}_{}{}^{\ensuremath{-}3.3}$, and $E_{\mathrm{c}.\mathrm{m}.}^{}{}_{}{}^{\ensuremath{-}9.3}$, respectively. The differential cross sections are presented at 11 beam momenta. A peripheral peak is the dominant feature of the reactions ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0}$ and ${\ensuremath{\Sigma}}^{0}{K}^{0}$, for which ${K}^{*}$ exchange is allowed, but no such peaking is seen in ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}{\ensuremath{\Sigma}}^{\ensuremath{-}}{K}^{+}$. An exponential fit to the momentum-transfer distributions in the peripheral region yields slope parameters in the 6- to $10\ensuremath{-}{(\frac{\mathrm{BeV}}{c})}^{\ensuremath{-}2}$ range. The differential cross sections for ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0} \mathrm{and} {\ensuremath{\Sigma}}^{\ensuremath{-}}{K}^{+}$ show peaking for forward production of hyperons in the c.m. system, to which baryon exchange is expected to contribute. The angular distribution of the $\ensuremath{\Lambda}$ polarization in ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0}$ is presented.
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The reactions ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0},{\ensuremath{\Sigma}}^{0}{K}^{0}$, and ${\ensuremath{\Sigma}}^{\ensuremath{-}}{K}^{+}$ in the 1.5- to 4.2-$\frac{\mathrm{BeV}}{c}$ momentum range were studied in the Lawrence Radiation Laboratory's 72-in. hydrogen bubble chamber. The total cross sections for the three reactions decrease as $E_{\mathrm{c}.\mathrm{m}.}^{}{}_{}{}^{\ensuremath{-}3.6}$, $E_{\mathrm{c}.\mathrm{m}.}^{}{}_{}{}^{\ensuremath{-}3.3}$, and $E_{\mathrm{c}.\mathrm{m}.}^{}{}_{}{}^{\ensuremath{-}9.3}$, respectively. The differential cross sections are presented at 11 beam momenta. A peripheral peak is the dominant feature of the reactions ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0}$ and ${\ensuremath{\Sigma}}^{0}{K}^{0}$, for which ${K}^{*}$ exchange is allowed, but no such peaking is seen in ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}{\ensuremath{\Sigma}}^{\ensuremath{-}}{K}^{+}$. An exponential fit to the momentum-transfer distributions in the peripheral region yields slope parameters in the 6- to $10\ensuremath{-}{(\frac{\mathrm{BeV}}{c})}^{\ensuremath{-}2}$ range. The differential cross sections for ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0} \mathrm{and} {\ensuremath{\Sigma}}^{\ensuremath{-}}{K}^{+}$ show peaking for forward production of hyperons in the c.m. system, to which baryon exchange is expected to contribute. The angular distribution of the $\ensuremath{\Lambda}$ polarization in ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}\ensuremath{\Lambda}{K}^{0}$ is presented.
Key concepts: Computer science