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Nonmesonic Weak Decay of $\Lambda$ Hypernuclei: The Three--Nucleon Induced Mode

机译:$ \ Lambda $ Hypernuclei的Nonmesonic弱衰变:三核   诱导模式

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摘要

The nonmesonic weak decay of $\Lambda$ hypernuclei is studied within amicroscopic diagrammatic approach which is extended to include thethree--nucleon induced mechanism. We adopt a nuclear matter formalism which,through the local density approximation, allows us to model finite hypernuclei,a one--meson--exchange weak transition potential and a Bonn nucleon--nucleonstrong potential. One--, two-- and three--nucleon induced weak decay rates arepredicted for $^{12}_\Lambda$C by including ground state correlations up tosecond order in the nucleon--nucleon potential and the recoil of the residualnucleus. Three--nucleon stimulated decays, $\Lambda NNN\to nNNN$ ($N=n$ or$p$), are considered here for the first time. The obtained decay rates comparewell with the latest KEK and FINUDA data. The three--nucleon induced rate turnsout to be dominated by $nnp$-- and $npp$--induced decays, it amounts to $\sim$7\% of the total nonmesonic rate and it is $\sim 1/2$ of the neutron--induceddecay rate. The reduction effect of the nuclear recoil is particularly relevantfor the three--nucleon induced rates ($\sim$ 15\%), less important for thetwo--nucleon induced rates ($\sim$ 4\%) and negligible for the one--nucleoninduced rates. Given the non--negligible size of the three--nucleon inducedcontribution and consequently its importance in the precise determination ofthe complete set of decay rates, new measurements and/or experimental analysisare encouraged.
机译:在显微镜图解法中研究了$ \ Lambda $超核的非中子弱衰变,该方法扩展到包括三个核子诱导的机制。我们采用核物质形式主义,通过局部密度近似,我们可以对有限的超核建模,即一个单介子交换弱跃迁势和一个波恩核子强核势。通过在核子-核子电势和残留核的后坐力中包含高达第二阶的基态相关性,可预测$ ^ {12} _ \ Lambda $ C的一,二和三核子诱导的弱衰变率。在这里首次考虑了三核子受激衰变$ \ Lambda NNN \至nNNN $($ N = n $或$ p $)。获得的衰减率与最新的KEK和FINUDA数据进行比较。三个由核子引起的速率结果主要由$ nnp $和$ npp $引起的衰变所主导,其总计为$ \ sim $ 7 \%的总非介子速率,为$ \ sim 1/2 $中子诱发的衰变率核后坐力的减少效果与三核子诱发率($ \ sim $ 15%)尤其相关,对三核子诱发率($ sim $ 4 \%)的重要性较小,而对其中一种可以忽略不计-核苷诱导的速率。鉴于三核子诱导贡献的大小不可忽略,因此在精确确定完整的衰变速率集合中的重要性,鼓励进行新的测量和/或实验分析。

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