Production of $\nu_{\tau}$ neutrinos and ${\overline \nu}_{\tau}$ antineutrinos - elaborate calculation for a fixed target experiment SHiP

R. Maciuła
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Abstract

We discuss cross sections for $\nu_{\tau}$ and ${\overline \nu}_{\tau}$ production from the direct $D_s^{\pm} \to \nu_{\tau}/{\overline \nu}_{\tau}$ and chain $D_s^{\pm} \to \tau^+/\tau^- \to \nu_{\tau}/{\overline \nu}_{\tau}$ decays in $p\!+^{96}\!\mathrm{Mo}$ scattering with proton beam $E_{\mathrm{lab}}$ = 400 GeV \textit{i.e.} at $\sqrt{s}_{NN}$ = 27.4 GeV. In our calculations we include $D_s^{\pm}$ from charm fragmentation $c \to D_s^{+}$ and $\bar c \to D_s^-$ as well as those from subleading fragmentation of strange quarks/antiquarks $s \to D_s^-$ and $\bar s \to D_s^+$. The different contributions to $D_s^{\pm}$ and $\nu_{\tau} / {\overline \nu}_{\tau}$ production rates are shown explicitly. Estimates of a number of observed $\nu_{\tau} / \overline{\nu}_{\tau}$ in the $\nu_{\tau} / \overline{\nu}_{\tau} +^{208}\!\mathrm{Pb}$ reaction, with 2m long target are given.
$\nu_{\tau}$中微子和${\overline \nu}_{\tau}$反中微子的产生——固定目标实验船的详细计算
我们讨论了在质子束$E_{\mathrm{lab}}$ = 400 GeV\textit{即}$\sqrt{s}_{NN}$ = 27.4 GeV的$p\!+^{96}\!\mathrm{Mo}$散射下,直接$D_s^{\pm} \to \nu_{\tau}/{\overline \nu}_{\tau}$和链$D_s^{\pm} \to \tau^+/\tau^- \to \nu_{\tau}/{\overline \nu}_{\tau}$衰变产生$\nu_{\tau}$和${\overline \nu}_{\tau}$的截面。在我们的计算中,我们包括了符号化碎片$c \to D_s^{+}$和$\bar c \to D_s^-$的$D_s^{\pm}$,以及奇异夸克/反夸克子碎片$s \to D_s^-$和$\bar s \to D_s^+$的。对$D_s^{\pm}$和$\nu_{\tau} / {\overline \nu}_{\tau}$生产率的不同贡献被明确地显示出来。给出了在目标长度为2米的$\nu_{\tau} / \overline{\nu}_{\tau} +^{208}\!\mathrm{Pb}$反应中所观察到的$\nu_{\tau} / \overline{\nu}_{\tau}$数的估计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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