Distinguishing Non-Standard Interaction and Lorentz Invariance Violation at Protvino to Super-ORCA experiment

Majhi, Rudra; Singha, Dinesh Kumar; Ghosh, Monojit; Mohanta, Rukmani

doi:10.48550/arxiv.2212.07244

Cited by 1 publication

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“…None of these experiments found any positive signal of LIV and set competitive bounds on various LIV parameters. In addition to the aforementioned studies by the experimental collaborations, there are various independent works towards the exploration of LIV with accelerator neutrinos in long-baseline experiments [48,50,[60][61][62][63][64][65][66][67][68], reactor antineutrinos in short-baseline experiments [69], atmospheric neutrinos [70][71][72][73][74], solar neutrinos [75], and high-energy neutrinos from astrophysical sources [76][77][78]. Recently, the KATRIN experi-ment, using the data from the first scientific run, placed limits on some of the oscillationfree LIV parameters that can not be probed by the time-of-flight or neutrino oscillation experiments [79].…”

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confidence: 99%

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

Agarwalla¹,

Das²,

Sahoo³

et al. 2023

Preprint

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Unified theories such as string theory and loop quantum gravity allow the Lorentz Invariance Violation (LIV) at the Planck Scale (M P ∼ 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 ∼ 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 longbaseline 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 appearance (ν µ → ν e ) and disappearance (ν µ → ν 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 and the most uncertain 3ν oscillation parameters, namely, θ 23 and δ CP . We find that for non-maximal values of θ 23 (θ 23 = 45 • ), 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 upper bounds on these CPTviolating 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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