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首页> 外文期刊>The European Physical Journal, A. Hadrons and Nuclei >Lambda hyperon production and polarization in collisions of p(3.5 GeV)+Nb
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Lambda hyperon production and polarization in collisions of p(3.5 GeV)+Nb

机译:p(3.5 GeV)+ Nb碰撞中的Lambda超子产生和极化

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摘要

Results on Λ hyperon production are reported for collisions of p(3.5 GeV) + Nb, studied with the High-Acceptance Di-Electron Spectrometer (HADES) at SIS18 at GSI Helmholtzzentrum for Heavy-Ion Research, Darmstadt. The transverse mass distributions in rapidity bins are well described by Boltzmann shapes with a maximum inverse slope parameter of about 90MeV at a rapidity of y = 1.0, i.e. slightly below the center-of-mass rapidity for nucleon-nucleon collisions, ycm = 1.12. The rapidity density decreases monotonically with increasing rapidity within a rapidity window ranging from 0.3 to 1.3. The Λ phasespace distribution is compared with results of other experiments and with predictions of two transport approaches which are available publicly. None of the present versions of the employed models is able to fully reproduce the experimental distributions, i.e. in absolute yield and in shape. Presumably, this finding results from an insufficient modelling in the transport models of the elementary processes being relevant for Λ production, rescattering and absorption. The present high-statistics data allow for a genuine twodimensional investigation as a function of phase space of the self-analyzing Λ polarization in the weak decay Λ → pπ~-. Finite negative values of the polarization in the order of 5-20% are observed over the entire phase space studied. The absolute value of the polarization increases almost linearly with increasing transverse momentum for p_t > 300MeV/c and increases with decreasing rapidity for y < 0.8.
机译:报告了p(3.5 GeV)+ Nb碰撞的Λ超子产生的结果,该结果由位于达姆施塔特GSI Helmholtzzentrum的重离子研究GSI Helmholtzzentrum的高接受双电子谱仪(HADES)研究。速度仓中的横向质量分布很好地由Boltzmann形状描述,在y = 1.0的速度下,最大反斜率参数约为90MeV,即略低于核子-核子碰撞的质子速度中心ycm = 1.12。速度密度在0.3到1.3的速度窗口内随着速度的增加而单调降低。将相空间分布与其他实验的结果以及公开提供的两种传输方法的预测进行比较。所用模型的当前版本均不能完全再现实验分布,即绝对产量和形状。据推测,该发现是由于基本过程的传输模型中与Λ的产生,再散射和吸收有关的建模不足所致。当前的高统计数据允许进行真正的二维研究,作为在弱衰减Λ→pπ〜-中自分析Λ极化的相空间的函数。在研究的整个相空间中观察到偏振的负值约为5-20%。当p_t> 300MeV / c时,极化的绝对值几乎随线性动量的增加而线性增加,而对于y <0.8,极化的绝对值随速度的减小而增加。

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