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  • Open Access

Comprehensive study of Lorentz invariance violation in atmospheric and long-baseline experiments

Deepak Raikwal, Sandhya Choubey, and Monojit Ghosh
Phys. Rev. D 107, 115032 – Published 28 June 2023

Abstract

In this paper, we have presented a comprehensive study of Lorentz invariance violation (LIV) in the context of the atmospheric neutrino experiment ICAL and the long-baseline experiments T2HK and DUNE. Our study consists of the full parameter space of the LIV parameters, i.e., six CPT-violating LIV parameters (aαβ) and six CPT-conserving LIV parameters (cαβ). In this study, our objective is to calculate the upper bound on all the LIV parameters with respect to the individual experiments as well as their combination. Our results show that DUNE gives the best sensitivity for the parameters aee, aeμ, aeτ, and aμτ in its 7 years of running, whereas ICAL gives the best sensitivity on aμμ, aμτ, cee, cμμ, cττ, and cμτ in its 10 years of running. For aττ, the sensitivities of DUNE and ICAL are almost same. The combination of T2HK, DUNE, and ICAL gives the best sensitivity for aeμ and aee with respect to all the existing bounds in the literature. For the CPT-even diagonal parameters cee and cμμ, our work provides the first-ever bounds.

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  • Received 10 April 2023
  • Accepted 5 June 2023

DOI:https://doi.org/10.1103/PhysRevD.107.115032

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

  1. Physical Systems
Particles & Fields

Authors & Affiliations

Deepak Raikwal*

  • Harish-Chandra Research Institute, A CI of Homi Bhabha National Institute, Chhatnag Road, Jhunsi, Prayagraj–211019, India and Homi Bhabha National Institute, Anushakti Nagar, Mumbai 400094, India

Sandhya Choubey

  • Department of Physics, School of Engineering Sciences, KTH Royal Institute of Technology, AlbaNova University Center, Roslagstullsbacken 21, SE–106 91 Stockholm, Sweden and The Oskar Klein Centre, AlbaNova University Center, Roslagstullsbacken 21, SE–106 91 Stockholm, Sweden

Monojit Ghosh

  • Center of Excellence for Advanced Materials and Sensing Devices, Ruder Bošković Institute, 10000 Zagreb, Croatia

  • *deepakraikwal@hri.res.in
  • choubey@kth.se
  • mghosh@irb.hr

Article Text

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Issue

Vol. 107, Iss. 11 — 1 June 2023

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Images

  • Figure 1
    Figure 1

    Probability oscillogram for ΔPνμνμ and ΔPν¯μν¯μ channels for aee, aμμ, aττ, aeμ, aeτ, and aμτ. For ICAL, the relevant energy region of the oscillograms is 1–100 GeV. The red line shows the region relevant for DUNE and the black line shows the region relevant for T2HK.

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  • Figure 2
    Figure 2

    Probability oscillograms for ΔPνμνμ and ΔPν¯μν¯μ channels for cee, cμμ, cττ, ceμ, ceτ, and cμτ. For ICAL, the relevant energy region of the oscillograms is 1–100 GeV. The red line shows the region relevant for DUNE and the black line shows the region relevant for T2HK.

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  • Figure 3
    Figure 3

    The νe appearance probability plots for aee, aμμ, aττ (first/second row is for δCP=0°/90°) and aeμ, aeτ, aμτ (third/fourth row is for δCP=0°/90°) for DUNE setup. In all panels the probabilities for standard three generation oscillations are shown by the solid black curves.

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  • Figure 4
    Figure 4

    The νe appearance probability plots for cee, cμμ, cττ (first/second row is for δCP=0°/90°) and ceμ, ceτ, cμτ (third/fourth row is for δCP=0°/90°) for DUNE setup. In all panels the probabilities for standard three generation oscillations are shown by the solid black curves.

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  • Figure 5
    Figure 5

    The νe appearance probability plots for aee, aμμ, aττ (first/second row is for δCP=0°/90°) and aeμ, aeτ, aμτ (third/fourth row is for δCP=0°/90°) for T2HK setup. In all panels the probabilities for standard three generation oscillations are shown by the solid black curves.

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  • Figure 6
    Figure 6

    χ2 as a function of LIV parameters aee, aμμ, and aττ for true δCP=0° (left column) and 90° (right column) in ICAL, DUNE, T2HK and combined.

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  • Figure 7
    Figure 7

    95% C.L. (2 dof) contour plots between |aαβ| and ϕαβa. Left column is for δCP=0° and right column is for δCP=90°.

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  • Figure 8
    Figure 8

    χ2 as a function of LIV parameters cee, cμμ, and cττ for true δCP=0° (left column) and 90° (right column) in ICAL, DUNE and combined.

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  • Figure 9
    Figure 9

    95% C.L. (2 dof) contour plots between |cαβ| and ϕαβc. Left column is for δCP=0° and right column is for δCP=90°.

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  • Figure 10
    Figure 10

    In the left panel, we have shown our limit for CPT-odd parameters (red bars) and current best bounds (green bars) which are listed in Table 5. In right panel, we have shown results for CPT-even parameters. Note that the current bound for cττ is at 90% C.L whereas all the other bounds are at 95% C.L.

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