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arXiv 2302.12005hep-phhep-exphysics.ins-det
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利用下一代长基线实验约束洛伦兹不变性破缺

Constraining Lorentz Invariance Violation with Next-Generation Long-Baseline Experiments

Sanjib Kumar Agarwalla, Sudipta Das, Sadashiv Sahoo, Pragyanprasu Swain

AI总结:

本文系统研究了下一代长基线实验 DUNE 和 T2HK 对 CPT 破坏型与守恒型洛伦兹不变性破缺参数的约束能力,推导了解析概率表达式,分析了参数简并性,并给出单独及联合实验在 95% 置信水平下的预期限制。

摘要:

弦理论和圈量子引力等统一理论允许在普朗克尺度($M_P \sim 10^{19}$ GeV)上发生洛伦兹不变性破缺(LIV)。利用有效场论,这种效应可以在低能下以强度约为 $\sim 1/M_P$ 的新相互作用形式被观测到。这些新相互作用包含带有 LIV 系数的算符,这些系数可以是 CPT 破坏型的,也可以是 CPT 守恒型的。在这项工作中,我们详细研究了这些 LIV 参数如何改变下一代长基线实验 DUNE 和 T2HK 中的跃迁概率。我们分别评估了这些实验单独以及联合时对非对角 CPT 破坏型($a_{e\mu}$、$a_{e\tau}$、$a_{\mu\tau}$)和 CPT 守恒型($c_{e\mu}$、$c_{e\tau}$、$c_{\mu\tau}$)LIV 参数的约束灵敏度。我们推导了在这些 LIV 参数存在时 $\nu_\mu\to\nu_e$ 和 $\nu_\mu\to\nu_\mu$ 概率的近似紧凑解析表达式,以解释我们的数值结果。我们探索了这些 LIV 参数与 3$\nu$ 参数 $\theta_{23}$ 和 $\delta_{\rm CP}$ 之间可能存在的相关性和简并性。我们发现,对于 $\theta_{23}$ 的非极大值,单独的 DUNE 和 T2HK 在其相反八分圆中存在简并解。当我们将 DUNE 和 T2HK 的数据结合时,这些简并性消失。在无信号的情况下,我们使用单独的 DUNE、T2HK 及其组合,在 95% 置信水平上给出了对这些 CPT 破坏型和 CPT 守恒型 LIV 参数的预期限制。我们观察到,由于 DUNE 能够利用更长的基线和更高能量的中微子,与 T2HK 相比,它在探测所有这些 LIV 参数方面具有更好的能力。由于包含 CPT 守恒型 LIV 参数的项在振荡概率中与中微子能量成正比,而 T2HK 主要处理亚 GeV 中微子,因此 T2HK 对 CPT 守恒型 LIV 参数几乎不敏感。

英文摘要:

Unified theories such as string theory and loop quantum gravity allow the Lorentz Invariance Violation (LIV) at the Planck Scale ($M_P \sim 10^{19}$ GeV). Using an effective field theory, this effect can be observed at low energies in terms of new interactions with a strength of $\sim 1/M_P$. These new interactions contain operators with LIV coefficients which can be CPT-violating or CPT-conserving. In this work, we study in detail how these LIV parameters modify the transition probabilities in the next-generation long-baseline experiments, DUNE and T2HK. We evaluate the sensitivities of these experiments in isolation and combination to constrain the off-diagonal CPT-violating ($a_{eμ}$, $a_{eτ}$, $a_{μτ}$) and CPT-conserving ($c_{eμ}$, $c_{eτ}$, $c_{μτ}$) LIV parameters. We derive approximate compact analytical expressions of $ν_μ\toν_e$ and $ν_μ\toν_μ$ probabilities in the presence of these LIV parameters to explain our numerical results. We explore the possible correlations and degeneracies between these LIV parameters & 3$ν$ parameters $θ_{23}$ & $δ_{\rm CP}$. We find that for non-maximal values of $θ_{23}$, there exist degenerate solutions in its opposite octant for standalone DUNE and T2HK. These degeneracies disappear when we combine the data from DUNE and T2HK. In case of no-show, we place the expected bounds on these CPT-violating and CPT-conserving LIV parameters at 95% C.L. using the standalone DUNE, T2HK, and their combination. We observe that due to its access to a longer baseline and high-energy neutrinos, DUNE has a better reach in probing all these LIV parameters as compared to T2HK. Since the terms containing the CPT-conserving LIV parameters are proportional to neutrino energy in oscillation probabilities, T2HK is almost insensitive to the CPT-conserving LIV parameters because it mostly deals with sub-GeV neutrinos.

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