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arXiv 2202.07539hep-phnucl-th
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(反)中微子核散射中可见光运动学的τ纵、横极化

Tau longitudinal and transverse polarizations from visible kinematics in (anti-)neutrino nucleus scattering

E. Hernández, J. Nieves, F. Sánchez, J. E. Sobczyk

摘要:

由于$ν_τ(\barν_τ) A_Z \to τ^\mp X$反应是出了名的难以直接测量,关于这个核过程的动力学的信息应该从τ衰变可见产物的能量和角分布的分析中提取。这些分布取决于τ偏振矢量的分量。首次给出了$ν_τA_Z \to τ^-(π^- ν_τ, ρ^-ν_τ) X$和$\barν_τA_Z \to τ^+(π^+ \barν_τ, ρ^+ \barν_τ) X$序贯反应的强子(π介子或ρ介子)出射能量和角微分截面的一般表达式。尽管所有可能的核反应机制都对分布有贡献,但通过实施适当的选择标准,有可能分离/增强其中之一。对于氧和中微子能量低于6 GeV的准弹性反应的情况下,我们表明,π介子分布的τ-极化分量的细节是敏感的。我们发现之间的显着差异的完整的计算,其中的纵向和横向分量的τ偏振矢量随能量和所产生的τ的散射角,和简化的计划,其中的偏振被设置为一个和零(各自的渐近值在高能量制度)。除了对中微子振荡分析的潜在影响外,这一结果还可用于进一步检验不同的核模型,因为这些观测量提供了与通过包容性核弱带电电流微分截面获得的信息互补的信息。我们还研究了对$W_4$、$W_5$原子核结构函数截面的影响,这些函数的贡献与带电轻子质量成正比,因此在μ子和电子中微子实验中难以约束。

英文摘要:

Since the $ν_τ(\barν_τ) A_Z \to τ^\mp X$ reaction is notoriously difficult to be directly measured, the information on the dynamics of this nuclear process should be extracted from the analysis of the energy and angular distributions of the tau decay visible products. These distributions depend on the components of the tau-polarization vector. We give, for the first time, the general expression for the outgoing hadron (pion or rho meson) energy and angular differential cross section for the sequential $ν_τA_Z \to τ^-(π^- ν_τ, ρ^-ν_τ) X$ and $\barν_τA_Z \to τ^+(π^+ \barν_τ, ρ^+ \barν_τ) X$ reactions. Though all possible nuclear reaction mechanisms contribute to the distribution, it may be possible to isolate/enhance one of them by implementing appropriate selection criteria. For the case of the quasi-elastic reaction off oxygen and neutrino energies below 6 GeV, we show that the pion distributions are sensitive to the details of the tau-polarization components. We find significant differences between the full calculation, where the longitudinal and transverse components of the tau polarization vector vary with the energy and the scattering angle of the produced tau, and the simplified scheme in which the polarizations are set to one and zero (respective asymptotic values in the high energy regime). In addition to its potential impact on neutrino oscillation analyses, this result can be used to further test different nuclear models, since these observables provide complementary information to that obtained by means of the inclusive nuclear weak charged-current differential cross section. We also study the effects on the cross section of the $W_4$, $W_5$ nuclear structure functions, which contributions are proportional to the charged lepton mass, and therefore difficult to constrain in muon and electron neutrino experiments.

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