通过部分波分析确定在$overline{p}p$湮灭中产生的$Ξ(1690)^-$和$Ξ(1820)^-$的自旋

Deepak Pachattu
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引用次数: 0

摘要

最近[arXiv:2201.03852v2]PANDA合作研究了确定$\Xi(1690)^{-}$和$\Xi(1820)^{-}$共振在$\Lambda K^-$体系中的自旋和奇偶性的可行性,这些共振是在$\bar{p}p$碰撞中产生的,反应通道为$\overline{p} p \rightarrow \bar{\Xi}^{+} \Lambda K^{-}$。这一贡献旨在利用早先开发的与模型无关的可还原张量形式主义来研究这些反应。如果 $\Xi(1690)^{-}$ 或$\Xi(1820)^{-}$ 的自旋为-1/2,只要这些共振是在阈值处产生的(s 波产生),那么部分波幅就是零。
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Partial-wave analysis to determine the spin of $Ξ(1690)^-$ and $Ξ(1820)^-$ produced in $\overline{p}p$ annihilation
Recently [arXiv:2201.03852v2] the PANDA collaboration studied the feasibility of determining the spin and parity of the $\Xi(1690)^{-}$and $\Xi(1820)^{-}$ resonances in the $\Lambda K^-$ system produced in $\bar{p}p$ collisions via the reaction channel $\overline{p} p \rightarrow \bar{\Xi}^{+} \Lambda K^{-}$. This contribution aims to study these reactions using a model-independent irreducible tensor formalism developed earlier. This study leads us to identify the partial-wave amplitude, which would be zero if $\Xi(1690)^{-}$ or $\Xi(1820)^{-}$ had spin-1/2, provided these resonances are produced at threshold (s-wave production).
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