pith. sign in

arxiv: 1907.01185 · v1 · pith:BRSTFIWGnew · submitted 2019-07-02 · ✦ hep-ph · hep-ex

Neutrino oscillations at dual baselines

Pith reviewed 2026-05-25 11:27 UTC · model grok-4.3

classification ✦ hep-ph hep-ex
keywords neutrino oscillationsdual baselinemass hierarchyCP phaseT2HKKlong-baseline experiments
0
0 comments X

The pith

A new parameter that exploits correlations between neutrino oscillations at two different baselines helps resolve the mass hierarchy and CP phase.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines the benefits of placing detectors at two separate baselines in long-baseline neutrino experiments rather than one. It introduces a correlation parameter that links the oscillation patterns observed at each baseline. Analysis of the proposed T2HKK setup shows this parameter reduces ambiguity when extracting the neutrino mass hierarchy and the CP-violating phase. The approach is presented as applicable to any dual-baseline configuration.

Core claim

By defining a new parameter that captures the shared information between oscillation probabilities at two baselines, the dual-baseline data improves the ability to determine the mass hierarchy and the CP phase compared with single-baseline analyses alone.

What carries the argument

The correlation parameter between the two baseline oscillation signals, which encodes their joint dependence on the hierarchy and CP phase.

If this is right

  • Mass hierarchy determination gains from the joint baseline information in any dual-baseline setup.
  • The CP phase can be constrained more tightly when the correlation between the two oscillation channels is used.
  • The method applies without requiring additional detectors beyond the two baselines.
  • Results extend to other future experiments that adopt two baselines.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The correlation approach might allow experiments to reach the same precision with lower total exposure than single-baseline designs.
  • It could be combined with atmospheric neutrino data to cross-check hierarchy results.
  • Future work could test whether the parameter remains useful when realistic energy resolution differences between sites are included.

Load-bearing premise

Systematic uncertainties and detector responses at the two sites must allow extraction of the shared correlation parameter without one site's effects overwhelming the joint information.

What would settle it

If re-analysis of T2HKK simulated data shows that adding the correlation parameter produces no gain in hierarchy or CP sensitivity beyond standard single-baseline fits, the claimed advantage does not hold.

Figures

Figures reproduced from arXiv: 1907.01185 by Hye-Sung Lee, Minseok Cho, Sushant K. Raut, YeolLin ChoeJo, Young-Min Lee.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: shows the energy dependence of Rdual for several values of δCP . Each value of δCP gives a characteristic series of spikes at the energies where Rdual diverge. Since the first zero for the 1100 km baseline lies around 1.2 GeV, there are no spikes above this energy. The diverging spikes would allow a high resolution in identifying the energies [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Contours indicate the points where the spikes of Fig. 2 at T2HKK occur. At these points, [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Locations of the [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
read the original abstract

Beam neutrino oscillation experiments typically employ only one detector at a certain baseline, apart from the near detector that measures the unoscillated neutrino flux at the source. Lately, there have been discussions of having detectors at two different baselines in one of the future long-baseline neutrino oscillation experiments. We study the potential advantage of a general dual-baseline system and perform analysis with a specific example of the envisioned T2HKK experiment. We introduce a new parameter to exploit the correlation between the oscillations at both baselines, and show how it can help in determining the mass hierarchy and the CP phase in the neutrino sector. Our study and findings can be generically used for any dual-baseline system.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript proposes a new correlation parameter for dual-baseline neutrino oscillation experiments, illustrated with the T2HKK setup, that exploits the relationship between oscillation probabilities at two baselines to help resolve degeneracies in the neutrino mass hierarchy and CP-violating phase. The approach is presented as generically applicable to any dual-baseline configuration.

Significance. If the central claim holds after accounting for experimental effects, the new parameter offers a methodological tool that could enhance sensitivity to hierarchy and CP phase in future long-baseline experiments by leveraging existing dual-baseline data correlations rather than requiring new hardware. The generic framing for any dual-baseline system is a positive feature.

major comments (2)
  1. [T2HKK analysis and results sections] The T2HKK analysis does not demonstrate robustness of the correlation parameter against site-specific systematic uncertainties (different detector responses, energy resolutions, and flux normalizations between the Japan and Korea sites). This is load-bearing for the central claim, as the skeptic's note correctly identifies that differing covariances would decorrelate the two measurements and erase the reported gain in hierarchy/CP sensitivity.
  2. [parameter definition and extraction procedure] No quantitative study is shown of how the new parameter behaves after marginalization over the full systematic covariance matrix that differs between the two baselines; the abstract states that the parameter 'can help' but the manuscript must establish that the correlation survives this marginalization rather than being assumed.
minor comments (2)
  1. Notation for the new correlation parameter should be defined explicitly with an equation number at first use to improve clarity for readers.
  2. Figure captions for oscillation probability plots should explicitly state the assumed systematic uncertainties and whether they are correlated or uncorrelated between baselines.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive feedback on our manuscript. The comments highlight important aspects of systematic uncertainties in dual-baseline analyses that require clarification and strengthening. We address each major comment below and outline the revisions we will make.

read point-by-point responses
  1. Referee: [T2HKK analysis and results sections] The T2HKK analysis does not demonstrate robustness of the correlation parameter against site-specific systematic uncertainties (different detector responses, energy resolutions, and flux normalizations between the Japan and Korea sites). This is load-bearing for the central claim, as the skeptic's note correctly identifies that differing covariances would decorrelate the two measurements and erase the reported gain in hierarchy/CP sensitivity.

    Authors: We agree that the current T2HKK results do not fully quantify the impact of site-specific systematics that differ between the two baselines. The manuscript presents the correlation parameter under the assumption of shared systematics, without a dedicated marginalization over independent covariance matrices for detector response, energy resolution, and flux normalization. To address this, the revised version will include a new subsection performing this marginalization and showing the resulting sensitivity to mass hierarchy and CP phase, both with and without the differing covariances. This will establish whether the reported gain persists under realistic conditions. revision: yes

  2. Referee: [parameter definition and extraction procedure] No quantitative study is shown of how the new parameter behaves after marginalization over the full systematic covariance matrix that differs between the two baselines; the abstract states that the parameter 'can help' but the manuscript must establish that the correlation survives this marginalization rather than being assumed.

    Authors: The referee correctly notes the absence of a quantitative demonstration that the correlation survives marginalization over baseline-dependent systematics. While the parameter is defined to exploit the relationship between the two oscillation probabilities, the extraction procedure in the current text does not explicitly vary the full covariance matrix. In the revision we will add this study, presenting the behavior of the parameter (including its uncertainty and correlation with hierarchy and delta_CP) after marginalization, thereby substantiating the abstract claim with explicit results rather than assumption. revision: yes

Circularity Check

0 steps flagged

No circularity; new parameter is an explicit analytical construction

full rationale

The paper introduces a correlation parameter defined directly from the dual-baseline oscillation probabilities to resolve hierarchy/CP degeneracies. This is presented as a constructed tool for analysis rather than a first-principles prediction or derivation that reduces to its own inputs. No self-citations, fitted inputs renamed as predictions, or uniqueness theorems are invoked as load-bearing steps. The central claim remains an independent phenomenological study of T2HKK-style setups and does not collapse by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The work relies on the standard three-flavor neutrino oscillation framework and assumptions about the T2HKK experimental configuration; no new free parameters or invented entities are introduced in the abstract.

axioms (1)
  • domain assumption Standard three-flavor neutrino oscillation framework and T2HKK detector assumptions hold.
    The analysis uses the conventional PMNS matrix and oscillation probabilities without deriving them.

pith-pipeline@v0.9.0 · 5652 in / 1075 out tokens · 31859 ms · 2026-05-25T11:27:15.559365+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

35 extracted references · 35 canonical work pages · 27 internal anchors

  1. [1]

    Neutrino oscillations at dual baselines

    The values of these parameters serve as discriminators between mod- els of new physics that predict the existence of tiny non-zero neutrino masses. Further, these scenarios can also affect oscillations through non-standard interactions (NSIs). Consequently there is a worldwide effort by the neutrino physics community towards measuring the os- cillation para...

  2. [2]

    Solving the neutrino parameter degeneracy by measuring the T2K off-axis beam in Korea

    K. Hagiwara, N. Okamura and K. i. Senda, Phys. Lett. B 637, 266 (2006) Erratum: [Phys. Lett. 5 B 641, 491 (2006)] doi:10.1016/j.physletb.2006.09.003, 10.1016/j.physletb.2006.04.041 [hep-ph/0504061]

  3. [3]

    Physics potential of T2KK: An extension of the T2K neutrino oscillation experiment with a far detector in Korea

    K. Hagiwara, N. Okamura and K. i. Senda, Phys. Rev. D 76, 093002 (2007) doi:10.1103/PhysRevD.76.093002 [hep-ph/0607255]

  4. [4]

    The earth matter effects in neutrino oscillation experiments from Tokai to Kamioka and Korea

    K. Hagiwara, N. Okamura and K. i. Senda, JHEP 1109, 082 (2011) doi:10.1007/JHEP09(2011)082 [arXiv:1107.5857 [hep-ph]]

  5. [5]

    Revisiting T2KK and T2KO physics potential and $\nu_\mu$ - $\bar{\nu}_\mu$ beam ratio

    K. Hagiwara, P. Ko, N. Okamura and Y. Takaesu, Eur. Phys. J. C 77, no. 3, 138 (2017) doi:10.1140/epjc/s10052- 017-4684-1 [arXiv:1605.02368 [hep-ph]]

  6. [6]

    Abe et al

    K. Abe et al. [Hyper-Kamiokande Collaboration], PTEP 2018, no. 6, 063C01 (2018) doi:10.1093/ptep/pty044 [arXiv:1611.06118 [hep-ex]]

  7. [7]

    Sensitivity of the T2HKK experiment to the non-standard interaction

    S. Fukasawa, M. Ghosh and O. Yasuda, Phys. Rev. D95, no. 5, 055005 (2017) doi:10.1103/PhysRevD.95.055005 [arXiv:1611.06141 [hep-ph]]

  8. [8]

    J. Liao, D. Marfatia and K. Whisnant, JHEP 1701, 071 (2017) doi:10.1007/JHEP01(2017)071 [arXiv:1612.01443 [hep-ph]]

  9. [9]

    Effect of systematics in the T2HK, T2HKK, and DUNE experiments

    M. Ghosh and O. Yasuda, Phys. Rev. D 96, no. 1, 013001 (2017) doi:10.1103/PhysRevD.96.013001 [arXiv:1702.06482 [hep-ph]]

  10. [10]

    S. K. Raut, Phys. Rev. D 96, no. 7, 075029 (2017) doi:10.1103/PhysRevD.96.075029 [arXiv:1703.07136 [hep-ph]]

  11. [11]

    Imprints of a light Sterile Neutrino at DUNE, T2HK and T2HKK

    S. Choubey, D. Dutta and D. Pramanik, Phys. Rev. D96, no. 5, 056026 (2017) doi:10.1103/PhysRevD.96.056026 [arXiv:1704.07269 [hep-ph]]

  12. [12]

    Y. Abe, Y. Asano, N. Haba and T. Yamada, Eur. Phys. J. C 77, no. 12, 851 (2017) doi:10.1140/epjc/s10052-017- 5294-7 [arXiv:1705.03818 [hep-ph]]

  13. [13]

    Ghosh and O

    M. Ghosh and O. Yasuda, arXiv:1709.08264 [hep-ph]

  14. [14]

    Spotlighting the sensitivities of T2HK,T2HKK and DUNE

    K. Chakraborty, K. N. Deepthi and S. Goswami, Nucl. Phys. B 937, 303 (2018) doi:10.1016/j.nuclphysb.2018.10.013 [arXiv:1711.11107 [hep-ph]]

  15. [15]

    Tanabashi et al

    M. Tanabashi et al. [Particle Data Group], Phys. Rev. D 98, no. 3, 030001 (2018). doi:10.1103/PhysRevD.98.030001

  16. [16]

    Global analysis of three-flavour neutrino oscillations: synergies and tensions in the determination of theta_23, delta_CP, and the mass ordering

    I. Esteban, M. C. Gonzalez-Garcia, A. Hernandez- Cabezudo, M. Maltoni and T. Schwetz, JHEP 1901, 106 (2019) doi:10.1007/JHEP01(2019)106 [arXiv:1811.05487 [hep-ph]]

  17. [17]

    The JHF-Kamioka neutrino project

    Y. Itow et al. [T2K Collaboration], hep-ex/0106019

  18. [18]

    D. S. Ayres et al. [NOvA Collaboration], hep- ex/0503053

  19. [19]

    Evidence for oscillation of atmospheric neutrinos

    Y. Fukuda et al. [Super-Kamiokande Collab- oration], Phys. Rev. Lett. 81, 1562 (1998) doi:10.1103/PhysRevLett.81.1562 [hep-ex/9807003]

  20. [20]

    Ahrens et al

    J. Ahrens et al. [IceCube Collaboration], Nucl. Phys. Proc. Suppl. 118, 388 (2003) doi:10.1016/S0920- 5632(03)01337-9 [astro-ph/0209556]

  21. [21]

    Physics Potential of a Long Baseline Neutrino Oscillation Experiment Using J-PARC Neutrino Beam and Hyper-Kamiokande

    K. Abe et al. [Hyper-Kamiokande Proto- Collaboration], PTEP 2015, 053C02 (2015) doi:10.1093/ptep/ptv061 [arXiv:1502.05199 [hep-ex]]

  22. [22]

    Acciarri et al

    R. Acciarri et al. [DUNE Collaboration], arXiv:1512.06148 [physics.ins-det]

  23. [23]

    Physics Potential of the ICAL detector at the India-based Neutrino Observatory (INO)

    S. Ahmed et al. [ICAL Collaboration], Pramana 88, no. 5, 79 (2017) doi:10.1007/s12043-017-1373-4 [arXiv:1505.07380 [physics.ins-det]]

  24. [24]

    JUNO Conceptual Design Report

    Z. Djurcic et al. [JUNO Collaboration], arXiv:1508.07166 [physics.ins-det]

  25. [25]

    E. K. Akhmedov, R. Johansson, M. Lindner, T. Ohls- son and T. Schwetz, JHEP 0404, 078 (2004) doi:10.1088/1126-6708/2004/04/078 [hep-ph/0402175]

  26. [26]

    Signatures of the genuine and matter-induced components of the CP violation asymmetry in neutrino oscillations

    J. Bernabu and A. Segarra, JHEP 1811, 063 (2018) doi:10.1007/JHEP11(2018)063 [arXiv:1807.11879 [hep- ph]]

  27. [27]

    Getting the best out of T2K and NOvA

    S. Prakash, S. K. Raut and S. U. Sankar, Phys. Rev. D 86, 033012 (2012) doi:10.1103/PhysRevD.86.033012 [arXiv:1201.6485 [hep-ph]]

  28. [28]

    Simulation of long-baseline neutrino oscillation experiments with GLoBES

    P. Huber, M. Lindner and W. Winter, Comput. Phys. Commun. 167, 195 (2005) doi:10.1016/j.cpc.2005.01.003 [hep-ph/0407333]

  29. [29]

    New features in the simulation of neutrino oscillation experiments with GLoBES 3.0

    P. Huber, J. Kopp, M. Lindner, M. Rolinec and W. Winter, Comput. Phys. Commun. 177, 432 (2007) doi:10.1016/j.cpc.2007.05.004 [hep-ph/0701187]

  30. [30]

    M. A. Acero et al. [NOvA Collaboration], Phys. Rev. D 98, 032012 (2018) doi:10.1103/PhysRevD.98.032012 [arXiv:1806.00096 [hep-ex]]

  31. [31]

    Search for CP violation in Neutrino and Antineutrino Oscillations by the T2K experiment with $2.2\times10^{21}$ protons on target

    K. Abe et al. [T2K Collaboration], Phys. Rev. Lett. 121, no. 17, 171802 (2018) doi:10.1103/PhysRevLett.121.171802 [arXiv:1807.07891 [hep-ex]]

  32. [32]

    Status of non-standard neutrino interactions

    T. Ohlsson, Rept. Prog. Phys. 76, 044201 (2013) doi:10.1088/0034-4885/76/4/044201 [arXiv:1209.2710 [hep-ph]]

  33. [33]

    Farzan and M

    Y. Farzan and M. Tortola, Front. in Phys. 6, 10 (2018) doi:10.3389/fphy.2018.00010 [arXiv:1710.09360 [hep-ph]]

  34. [34]

    Non-Standard Interactions in propagation at the Deep Underground Neutrino Experiment

    P. Coloma, JHEP 1603, 016 (2016) doi:10.1007/JHEP03(2016)016 [arXiv:1511.06357 [hep- ph]]

  35. [35]

    A. S. Joshipura and S. Mohanty, Phys. Lett. B 584, 103 (2004) doi:10.1016/j.physletb.2004.01.057 [hep- ph/0310210]