pith. sign in

arxiv: 2605.29105 · v1 · pith:2CODCII2new · submitted 2026-05-27 · ✦ hep-ph · astro-ph.HE· hep-ex

Visible inelasticity as a probe of tau flavor content of astrophysical neutrinos

Pith reviewed 2026-06-29 10:47 UTC · model grok-4.3

classification ✦ hep-ph astro-ph.HEhep-ex
keywords astrophysical neutrinostau neutrinosvisible inelasticityIceCubestarting tracksneutrino flavor compositionmuonic decays
0
0 comments X

The pith

Visible inelasticity of starting tracks in neutrino telescopes statistically separates tau neutrinos from muon neutrinos.

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

The paper investigates visible inelasticity in starting track events as a way to measure the tau component of astrophysical neutrino fluxes. It shows that muonic decays of tau leptons create tracks with higher visible inelasticity than muon neutrino charged-current interactions. Realistic IceCube simulations indicate this difference already allows competitive constraints on the tau-to-muon flux ratio using data in hand. The approach complements double-cascade searches and opens routes to source-specific flavor measurements.

Core claim

Muonic decays of tau leptons produce tracks with systematically larger visible inelasticity than those from muon neutrino charged-current interactions, potentially enabling statistical separation of the two flavors; using realistic IceCube exposures and detector performance, this observable already yields competitive sensitivity to the tau-to-muon flux ratio R_τμ achievable with existing data.

What carries the argument

The systematic difference in visible inelasticity between muonic tau lepton decays and direct muon neutrino interactions in starting track events.

If this is right

  • Competitive sensitivity to R_τμ already reachable with current IceCube exposures and performance.
  • Flavor composition measurements become possible for individual astrophysical neutrino sources.
  • Tau-enhanced source catalogs can be selected using the inelasticity observable.
  • The method provides a probe of potential physics beyond standard neutrino mixing via flavor ratios.
  • It serves as an immediately accessible complement to rare double-cascade signatures.

Where Pith is reading between the lines

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

  • Reanalysis of archival IceCube starting-track samples could yield an early tau-flavor constraint without new data taking.
  • The inelasticity separation might be combined with other observables to tighten overall flavor ratio bounds.
  • If the separation persists, similar techniques could be tested at next-generation neutrino telescopes with improved track reconstruction.
  • Source-by-source application could reveal whether any known neutrino emitters show anomalous tau content.

Load-bearing premise

Detector response simulations accurately capture the difference in visible inelasticity between tau muonic decays and muon neutrino interactions without significant bias.

What would settle it

IceCube data or updated simulations showing no measurable difference in the visible inelasticity distributions for the two event classes after accounting for backgrounds and systematics.

Figures

Figures reproduced from arXiv: 2605.29105 by Alex Y. Wen, Carlos A. Arg\"uelles, Sergio Palomares-Ruiz.

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: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: currently exceed the allowed region, as measure￾ments improve, Rτµ could become one of the most sen￾sitive probes of tau flavor, and any significant tension between measurement and theory would constitute ma￾jor evidence for beyond Standard Model (BSM) effects in the neutrino sector. A potential source of tau-flavored background are tau neutrinos from the prompt atmospheric flux. To assess their contributi… view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4 [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
read the original abstract

Astrophysical neutrinos provide a unique probe of neutrino flavor changes over cosmological baselines. While the tau component of the neutrino flux is expected to arise almost entirely from mixing, current measurements rely primarily on rare double-cascade signatures. We investigate a complementary method to measure the tau fraction using the visible inelasticity of starting track events in neutrino telescopes. Muonic decays of tau leptons produce tracks with systematically larger visible inelasticity than those from muon neutrino interactions, potentially enabling statistical separation of the two flavors. Using realistic IceCube exposures and detector performance, we show that this observable already yields competitive sensitivity to the tau-to-muon flux ratio, $R_{\tau\mu}$, achievable with existing data. This approach may further enable flavor measurements of individual sources and the selection of tau-enhanced source catalogs. Starting-track inelasticity thus provides a powerful and immediately accessible probe of astrophysical neutrino flavor and of potential physics beyond standard neutrino mixing.

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 paper proposes using the visible inelasticity distribution of starting-track events in IceCube to statistically separate the tau-neutrino component from the muon-neutrino component of the astrophysical flux. It argues that muonic tau decays produce tracks with systematically higher visible inelasticity than direct u_ u CC interactions, and claims that realistic IceCube exposures already yield competitive sensitivity to the flux ratio R_ au u.

Significance. If the simulated inelasticity separation is shown to be robust against detector-response systematics, the method would provide a complementary, high-statistics handle on astrophysical neutrino flavor that does not rely on the rare double-cascade topology. This could enable source-by-source flavor measurements and tests of standard mixing over cosmological baselines.

major comments (2)
  1. [§3] §3: The central claim that muonic tau-decay tracks exhibit systematically larger visible inelasticity than u_ u CC tracks rests entirely on Monte Carlo distributions; the manuscript provides no data-driven validation or quantitative estimate of bias from hadronic-shower modeling, muon energy-loss parametrization, or starting-track selection cuts.
  2. [§4] §4: The assertion of “competitive sensitivity … achievable with existing data” is presented without tabulated statistical power, systematic-error budget, or the precise exposure and effective-area values used in the calculation, so the reader cannot assess whether modest degradation of the separation power would render the result marginal rather than competitive.
minor comments (2)
  1. [Abstract] Abstract: the quantitative claim of competitive sensitivity is stated without any numerical result or uncertainty; a single sentence summarizing the expected precision on R_ au u would improve clarity.
  2. Notation: the symbol R_ au u is introduced without an explicit definition in terms of the individual flavor fluxes; adding the definition near first use would aid readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their thoughtful review and positive evaluation of the significance of our proposed method. We respond to the major comments point by point below.

read point-by-point responses
  1. Referee: [§3] §3: The central claim that muonic tau-decay tracks exhibit systematically larger visible inelasticity than ν_μ CC tracks rests entirely on Monte Carlo distributions; the manuscript provides no data-driven validation or quantitative estimate of bias from hadronic-shower modeling, muon energy-loss parametrization, or starting-track selection cuts.

    Authors: We agree that the analysis is simulation-based, as is common for such proposed methods given the current statistics. The separation arises from well-understood kinematics: in ν_τ CC interactions followed by muonic τ decay, the visible track energy includes the hadronic shower plus a muon from the decay, leading to higher inelasticity y_vis compared to ν_μ CC where the muon carries most of the energy. To address the concern, we will revise the manuscript to include quantitative estimates of systematic biases. Specifically, we will vary hadronic shower models (e.g., using different generators) and muon energy loss parameters within their uncertainties and report the impact on the separation significance. While a full data-driven validation is limited by the small number of astrophysical starting-track events, we will compare the MC to atmospheric neutrino data in the relevant energy range to validate the modeling. This will be added in a new subsection in §3. revision: partial

  2. Referee: [§4] §4: The assertion of “competitive sensitivity … achievable with existing data” is presented without tabulated statistical power, systematic-error budget, or the precise exposure and effective-area values used in the calculation, so the reader cannot assess whether modest degradation of the separation power would render the result marginal rather than competitive.

    Authors: We acknowledge that additional details would improve clarity. In the revised version, we will add a dedicated table summarizing the statistical power (e.g., expected significance for R_τμ =1), the systematic error budget (including contributions from flux normalization, detector systematics, and modeling uncertainties), and the precise exposure assumptions (e.g., livetime, effective area as function of energy). This will allow readers to evaluate the competitiveness under various scenarios. The calculations are based on 10 years of IceCube data with standard effective areas for starting tracks. revision: yes

Circularity Check

0 steps flagged

No significant circularity; sensitivity estimate uses independent Monte Carlo modeling of interaction physics

full rationale

The paper derives its sensitivity claim from Monte Carlo simulations of visible inelasticity distributions for tau muonic decays versus nu_mu CC interactions, using standard IceCube detector response modeling. This is an external input based on known particle physics and detector simulation, not a fit to the target R_tau_mu or a self-referential definition. No equations reduce the claimed separation power to a fitted parameter by construction, and no load-bearing self-citations or ansatze are present in the abstract or described sections. The derivation chain remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The approach rests on standard neutrino oscillation physics, tau decay branching ratios, and IceCube detector response modeling; no new free parameters or invented entities are introduced in the abstract.

axioms (2)
  • standard math Standard three-flavor neutrino mixing and tau lepton decay properties hold over astrophysical baselines
    Invoked to expect a non-zero tau component and to model the muonic decay channel.
  • domain assumption IceCube detector response simulations accurately reproduce visible inelasticity distributions for track events
    Required for the claim that the observable yields competitive sensitivity with existing data.

pith-pipeline@v0.9.1-grok · 5698 in / 1286 out tokens · 37157 ms · 2026-06-29T10:47:47.358961+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

98 extracted references · 87 canonical work pages · 54 internal anchors

  1. [1]

    M. G. Aartsenet al.(IceCube Collaboration), Evidence for high-energy extraterrestrial neutrinos at the IceCube detector, Science342, 1242856 (2013), arXiv:1311.5238 [astro-ph.HE]

  2. [2]

    J. G. Learned and S. Pakvasa, Detecting tau-neutrino os- cillations at PeV energies, Astropart. Phys.3, 267 (1995), arXiv:hep-ph/9405296

  3. [3]

    Probing Particle Physics with IceCube

    M. Ahlers, K. Helbing, and C. Pérez de los Heros, Prob- ing particle physics with IceCube, Eur. Phys. J. C78, 924 (2018), arXiv:1806.05696 [astro-ph.HE]

  4. [4]

    Fundamental Physics with High-Energy Cosmic Neutrinos

    M. Ackermannet al., Fundamental physics with high- energy cosmic neutrinos, Bull. Am. Astron. Soc.51, 215 (2019), arXiv:1903.04333 [astro-ph.HE]

  5. [5]

    C. A. Argüelles, M. Bustamante, A. Kheirandish, S. Palomares-Ruiz, J. Salvado, and A. C. Vincent, Fun- damental physics with high-energy cosmic neutrinos to- day and in the future, PoSICRC2019, 849 (2020), arXiv:1907.08690 [astro-ph.HE]

  6. [6]

    O. Mena, S. Palomares-Ruiz, and A. C. Vincent, Fla- vor composition of the high-energy neutrino events in IceCube, Phys. Rev. Lett.113, 091103 (2014), arXiv:1404.0017 [astro-ph.HE]

  7. [7]

    The spectrum and flavor composition of the astrophysical neutrinos in IceCube

    A. Watanabe, The spectrum and flavor composition of the astrophysical neutrinos in IceCube, JCAP08, 030, arXiv:1412.8264 [astro-ph.HE]

  8. [8]

    Spectral analysis of the high-energy IceCube neutrinos

    S. Palomares-Ruiz, A. C. Vincent, and O. Mena, Spectral analysisofthehigh-energyIceCubeneutrinos,Phys.Rev. D91, 103008 (2015), arXiv:1502.02649 [astro-ph.HE]

  9. [9]

    Which is the flavor of cosmic neutrinos seen by IceCube?

    A. Palladino, G. Pagliaroli, F. L. Villante, and F. Vis- sani, What is the flavor of the cosmic neutrinos seen by IceCube?, Phys. Rev. Lett.114, 171101 (2015), arXiv:1502.02923 [astro-ph.HE]

  10. [10]

    M. G. Aartsenet al.(IceCube Collaboration), Flavor ra- tio of astrophysical neutrinos above 35 TeV in IceCube, Phys. Rev. Lett.114, 171102 (2015), arXiv:1502.03376 [astro-ph.HE]

  11. [11]

    M. G. Aartsenet al.(IceCube Collaboration), A com- binedmaximum-likelihoodanalysisofthehigh-energyas- trophysical neutrino flux measured with IceCube, Astro- phys. J.809, 98 (2015), arXiv:1507.03991 [astro-ph.HE]

  12. [12]

    Mammen Abrahamet al., Tau neutrinos in the next decade: from GeV to EeV, J

    R. Mammen Abrahamet al., Tau neutrinos in the next decade: from GeV to EeV, J. Phys. G49, 110501 (2022), arXiv:2203.05591 [hep-ph]

  13. [13]

    Prospects for observations of high-energy cosmic tau neutrinos

    H. Athar, G. Parente, and E. Zas, Prospects for observa- tions of high-energy cosmic tau neutrinos, Phys. Rev. D 62, 093010 (2000), arXiv:hep-ph/0006123

  14. [14]

    P. F. de Salas, D. V. Forero, S. Gariazzo, P. Martínez- Miravé, O. Mena, C. A. Ternes, M. Tórtola, and J. W. F. Valle, 2020 global reassessment of the neutrino oscillation picture, JHEP02, 071, arXiv:2006.11237 [hep-ph]

  15. [15]

    NuFit-6.0: Updated global analysis of three-flavor neutrino oscillations

    I. Esteban, M. C. Gonzalez-Garcia, M. Maltoni, I. Martinez-Soler, J. P. Pinheiro, and T. Schwetz, NuFit- 6.0: updated global analysis of three-flavor neutrino os- cillations, JHEP12, 216, arXiv:2410.05380 [hep-ph]

  16. [16]

    Capozzi, W

    F. Capozzi, W. Giarè, E. Lisi, A. Marrone, A. Melchiorri, and A. Palazzo, Neutrino masses and mixing: Entering theeraofsubpercentprecision,Phys.Rev.D111,093006 (2025), arXiv:2503.07752 [hep-ph]

  17. [17]

    Flavor Composition and Energy Spectrum of Astrophysical Neutrinos

    P. Lipari, M. Lusignoli, and D. Meloni, Flavor compo- sition and energy spectrum of astrophysical neutrinos, Phys. Rev. D75, 123005 (2007), arXiv:0704.0718 [astro- ph]

  18. [18]

    Theoretically palatable flavor combinations of astrophysical neutrinos

    M. Bustamante, J. F. Beacom, and W. Winter, The- oretically palatable flavor combinations of astrophys- ical neutrinos, Phys. Rev. Lett.115, 161302 (2015), arXiv:1506.02645 [astro-ph.HE]

  19. [19]

    Ultra-high neutrino fluxes as a probe for non-standard physics

    A. Bhattacharya, S. Choubey, R. Gandhi, and A. Watan- abe, Ultra-high neutrino fluxes as a probe for non- standard physics, JCAP09, 009, arXiv:1006.3082 [hep- ph]

  20. [20]

    C. A. Argüelles, T. Katori, and J. Salvado, New physics in astrophysical neutrino flavor, Phys. Rev. Lett.115, 161303 (2015), arXiv:1506.02043 [hep-ph]

  21. [21]

    I. M. Shoemaker and K. Murase, Probing BSM neutrino physics with flavor and spectral distortions: prospects for future high-energy neutrino telescopes, Phys. Rev. D93, 085004 (2016), arXiv:1512.07228 [astro-ph.HE]

  22. [22]

    R. W. Rasmussen, L. Lechner, M. Ackermann, M. Kowal- ski, and W. Winter, Astrophysical neutrinos flavored with beyond the Standard Model physics, Phys. Rev. D 96, 083018 (2017), arXiv:1707.07684 [hep-ph]

  23. [23]

    N. Song, S. W. Li, C. A. Argüelles, M. Bustamante, and A. C. Vincent, The future of high-energy astro- physical neutrino flavor measurements, JCAP04, 054, arXiv:2012.12893 [hep-ph]

  24. [24]

    C. A. Argüelleset al., Snowmass white paper: beyond the standard model effects on neutrino flavor, Eur. Phys. J. C83, 15 (2023), arXiv:2203.10811 [hep-ph]

  25. [25]

    J. F. Beacom, N. F. Bell, D. Hooper, S. Pakvasa, and T. J. Weiler, Decay of high-energy astrophysical neu- trinos, Phys. Rev. Lett.90, 181301 (2003), arXiv:hep- ph/0211305

  26. [26]

    Testing neutrino flavor mixing plus decay with neutrino telescopes

    M. Maltoni and W. Winter, Testing neutrino oscilla- tions plus decay with neutrino telescopes, JHEP07, 064, arXiv:0803.2050 [hep-ph]

  27. [27]

    Neutrino Decays over Cosmological Distances and the Implications for Neutrino Telescopes

    P. Baerwald, M. Bustamante, and W. Winter, Neutrino decays over cosmological distances and the implications for neutrino telescopes, JCAP10, 020, arXiv:1208.4600 [astro-ph.CO]

  28. [28]

    Testing decay of astrophysical neutrinos with incomplete information

    M. Bustamante, J. F. Beacom, and K. Murase, Testing decay of astrophysical neutrinos with incom- plete information, Phys. Rev. D95, 063013 (2017), arXiv:1610.02096 [astro-ph.HE]

  29. [29]

    Abdullahi and P

    A. Abdullahi and P. B. Denton, Visible decay of astro- physical neutrinos at IceCube, Phys. Rev. D102, 023018 (2020), arXiv:2005.07200 [hep-ph]

  30. [30]

    R. M. Crocker, F. Melia, and R. R. Volkas, Search- ing for long wavelength neutrino oscillations in the dis- torted neutrino spectrum of galactic supernova rem- nants, Astrophys. J. Suppl.141, 147 (2002), arXiv:astro- 7 ph/0106090

  31. [31]

    J. F. Beacom, N. F. Bell, D. Hooper, J. G. Learned, S. Pakvasa, and T. J. Weiler, PseudoDirac neutrinos: a challenge for neutrino telescopes, Phys. Rev. Lett.92, 011101 (2004), arXiv:hep-ph/0307151

  32. [32]

    Pseudo-Dirac Neutrino Scenario: Cosmic Neutrinos at Neutrino Telescopes

    A. Esmaili, Pseudo-Dirac neutrino scenario: cosmic neu- trinos at neutrino telescopes, Phys. Rev. D81, 013006 (2010), arXiv:0909.5410 [hep-ph]

  33. [33]

    Carloni, I

    K. Carloni, I. Martínez-Soler, C. A. Arguelles, K. S. Babu, and P. S. B. Dev, Probing pseudo-Dirac neutri- nos with astrophysical sources at IceCube, Phys. Rev. D 109, L051702 (2024), arXiv:2212.00737 [astro-ph.HE]

  34. [34]

    Non-standard interaction effects on astrophysical neutrino fluxes

    M. Blennow and D. Meloni, Non-standard interaction ef- fects on astrophysical neutrino fluxes, Phys. Rev. D80, 065009 (2009), arXiv:0901.2110 [hep-ph]

  35. [35]

    M. C. Gonzalez-Garcia, M. Maltoni, I. Martinez-Soler, and N. Song, Non-standard neutrino interactions in the Earth and the flavor of astrophysical neutrinos, As- tropart. Phys.84, 15 (2016), arXiv:1605.08055 [hep-ph]

  36. [36]

    P. F. de Salas, R. A. Lineros, and M. Tórtola, Neutrino propagation in the galactic dark matter halo, Phys. Rev. D94, 123001 (2016), arXiv:1601.05798 [astro-ph.HE]

  37. [37]

    Flavor of cosmic neutrinos preserved by ultralight dark matter

    Y. Farzan and S. Palomares-Ruiz, Flavor of cosmic neu- trinos preserved by ultralight dark matter, Phys. Rev. D 99, 051702 (2019), arXiv:1810.00892 [hep-ph]

  38. [38]

    M. M. Reynoso, O. A. Sampayo, and A. M. Carulli, Neu- trino interactions with ultralight axion-like dark matter, Eur. Phys. J. C82, 274 (2022), arXiv:2203.11642 [hep- ph]

  39. [39]

    C. A. Argüelles, K. Farrag, and T. Katori, Ultra-light dark matter limits from astrophysical neutrino flavour, PoSICRC2023, 1415 (2023)

  40. [40]

    P. Q. Hung and H. Pas, Cosmo MSW effect for mass varying neutrinos, Mod. Phys. Lett. A20, 1209 (2005), arXiv:astro-ph/0311131

  41. [41]

    S. Ando, M. Kamionkowski, and I. Mocioiu, Neutrino oscillations, Lorentz/CPT violation, and dark energy, Phys. Rev. D80, 123522 (2009), arXiv:0910.4391 [hep- ph]

  42. [42]

    Effects of a neutrino-dark energy coupling on oscillations of high-energy neutrinos

    N. Klop and S. Ando, Effects of a neutrino-dark energy coupling on oscillations of high-energy neutrinos, Phys. Rev. D97, 063006 (2018), arXiv:1712.05413 [hep-ph]

  43. [43]

    Effects of neutrino mixing on high-energy cosmic neutrino flux

    H. Athar, M. Jezabek, and O. Yasuda, Effects of neutrino mixing on high-energy cosmic neutrino flux, Phys. Rev. D62, 103007 (2000), arXiv:hep-ph/0005104

  44. [44]

    Effects of sterile neutrinos on the ultrahigh-energy cosmic neutrino flux

    P. Keranen, J. Maalampi, M. Myyrylainen, and J. Riit- tinen, Effects of sterile neutrinos on the ultrahigh-energy cosmic neutrino flux, Phys. Lett. B574, 162 (2003), arXiv:hep-ph/0307041

  45. [45]

    C. A. Argüelles, K. Farrag, T. Katori, R. Khandelwal, S. Mandalia, and J. Salvado, Sterile neutrinos in astro- physicalneutrinoflavor,JCAP02,015,arXiv:1909.05341 [hep-ph]

  46. [46]

    Neutrino Observatories Can Characterize Cosmic Sources and Neutrino Properties

    G. Barenboim and C. Quigg, Neutrino observatories can characterize cosmic sources and neutrino properties, Phys. Rev. D67, 073024 (2003), arXiv:hep-ph/0301220

  47. [47]

    Lorentz and CPT Invariance Violation In High-Energy Neutrinos

    D. Hooper, D. Morgan, and E. Winstanley, Lorentz and CPT invariance violation in high-energy neutrinos, Phys. Rev. D72, 065009 (2005), arXiv:hep-ph/0506091

  48. [48]

    Diffuse Ultra-High Energy Neutrino Fluxes and Physics Beyond the Standard Model

    A. Bhattacharya, S. Choubey, R. Gandhi, and A. Watan- abe, Diffuse ultra-high energy neutrino fluxes and physics beyond the Standard Model, Phys. Lett. B690, 42 (2010), arXiv:0910.4396 [hep-ph]

  49. [49]

    Energy-independent new physics in the flavour ratios of high-energy astrophysical neutrinos

    M. Bustamante, A. M. Gago, and C. Pena-Garay, Energy-independent new physics in the flavour ratios of high-energy astrophysical neutrinos, JHEP04, 066, arXiv:1001.4878 [hep-ph]

  50. [50]

    Test of Lorentz Violation with Astrophysical Neutrino Flavor

    T. Katori, C. A. Argüelles, and J. Salvado, Test of Lorentz violation with astrophysical neutrino flavor, in 7th Meeting on CPT and Lorentz Symmetry(2017) pp. 209–212, arXiv:1607.08448 [hep-ph]

  51. [51]

    H.MinakataandA.Y.Smirnov,High-energycosmicneu- trinos and the equivalence principle, Phys. Rev. D54, 3698 (1996), arXiv:hep-ph/9601311

  52. [52]

    Probing Quantum Decoherence with High-Energy Neutrinos

    D. Hooper, D. Morgan, and E. Winstanley, Probing quantum decoherence with high-energy neutrinos, Phys. Lett. B609, 206 (2005), arXiv:hep-ph/0410094

  53. [53]

    L. A. Anchordoqui, H. Goldberg, M. C. Gonzalez-Garcia, F. Halzen, D. Hooper, S. Sarkar, and T. J. Weiler, Prob- ing Planck scale physics with IceCube, Phys. Rev. D72, 065019 (2005), arXiv:hep-ph/0506168

  54. [54]

    J. G. Learned, Dumand as a tau detector, inProceedings of the 1980 International DUMAND Symposium, Vol. 2, edited by V. J. Stenger (University of Hawaii / Hawaii DUMAND Center, Honolulu, Hawaii, 1981) p. 272

  55. [55]

    D. F. Cowen (IceCube), Tau neutrinos in IceCube, J. Phys. Conf. Ser.60, 227 (2007)

  56. [56]

    J. F. Beacom, N. F. Bell, D. Hooper, S. Pakvasa, and T. J. Weiler, Measuring flavor ratios of high-energy as- trophysical neutrinos, Phys. Rev. D68, 093005 (2003), [Erratum: Phys.Rev.D 72, 019901 (2005)], arXiv:hep- ph/0307025

  57. [57]

    Bugaev, T

    E. Bugaev, T. Montaruli, Y. Shlepin, and I. A. Sokalski, Propagation of tau neutrinos and tau leptons through the earth and their detection in underwater / ice neutrino telescopes, Astropart. Phys.21, 491 (2004), arXiv:hep- ph/0312295

  58. [58]

    Astrophysical tau neutrino detection in kilometer-scale Cherenkov detectors via muonic tau decay

    T. DeYoung, S. Razzaque, and D. F. Cowen, Astrophys- ical tau neutrino detection in kilometer-scale Cherenkov detectors via muonic tau decay, Astropart. Phys.27, 238 (2007), arXiv:astro-ph/0608486

  59. [59]

    S. W. Li, M. Bustamante, and J. F. Beacom, Echo tech- nique to distinguish flavors of astrophysical neutrinos, Phys. Rev. Lett.122, 151101 (2019), arXiv:1606.06290 [astro-ph.HE]

  60. [60]

    M. D. Kistler and R. Laha, Multi-PeV signals from a new astrophysical neutrino flux beyond the Glashow resonance, Phys. Rev. Lett.120, 241105 (2018), arXiv:1605.08781 [astro-ph.HE]

  61. [61]

    Abbasiet al.(IceCube Collaboration), Detection of astrophysical tau neutrino candidates in IceCube, Eur

    R. Abbasiet al.(IceCube Collaboration), Detection of astrophysical tau neutrino candidates in IceCube, Eur. Phys. J. C82, 1031 (2022), arXiv:2011.03561 [hep-ex]

  62. [62]

    Abbasiet al.(IceCube Collaboration), Observa- tion of seven astrophysical tau neutrino candidates with IceCube, Phys

    R. Abbasiet al.(IceCube Collaboration), Observa- tion of seven astrophysical tau neutrino candidates with IceCube, Phys. Rev. Lett.132, 151001 (2024), arXiv:2403.02516 [astro-ph.HE]

  63. [63]

    M. G. Aartsenet al.(IceCube Collaboration), The Ice- Cube neutrino observatory: instrumentation and online systems, JINST12(03), P03012, [Erratum: JINST 19, E05001 (2024)], arXiv:1612.05093 [astro-ph.IM]

  64. [64]

    Letter of Intent for KM3NeT 2.0

    S. Adrian-Martinezet al.(KM3NeT Collaboration), Let- ter of intent for KM3NeT 2.0, J. Phys. G43, 084001 (2016), arXiv:1601.07459 [astro-ph.IM]

  65. [65]

    Agostiniet al.(P-ONE Collaboration), The Pa- cific Ocean Neutrino Experiment, Nature Astron.4, 913 (2020), arXiv:2005.09493 [astro-ph.HE]

    M. Agostiniet al.(P-ONE Collaboration), The Pa- cific Ocean Neutrino Experiment, Nature Astron.4, 913 (2020), arXiv:2005.09493 [astro-ph.HE]. 8

  66. [66]

    A. D. Avrorinet al., Status and recent results of the BAIKAL-GVD project, Phys. Part. Nucl.46, 211 (2015)

  67. [67]

    Z. P. Yeet al.(TRIDENT Collaboration), A multi- cubic-kilometre neutrino telescope in the western Pacific Ocean, Nature Astron.7, 1497 (2023), arXiv:2207.04519 [astro-ph.HE]

  68. [68]

    C. A. Argüelleset al.(TAMBO Collaboration), TAMBO: A deep-valley neutrino observatory, (2025), arXiv:2507.08070 [astro-ph.HE]

  69. [69]

    A. N. Otte (Trinity Collaboration), The Trinity-one PeV-neutrino telescope, PoSICRC2025, 1136 (2025), arXiv:2509.18237 [astro-ph.HE]

  70. [70]

    The Giant Radio Array for Neutrino Detection (GRAND): Science and Design

    J. Álvarez-Muñizet al.(GRAND Collaboration), The Giant Radio Array for Neutrino Detection (GRAND): science and design, Sci. China Phys. Mech. Astron.63, 219501 (2020), arXiv:1810.09994 [astro-ph.HE]

  71. [71]

    Koteraet al.(BEACON and GRAND Collabora- tions), The Hybrid Elevated Radio Observatory for Neu- trinos (HERON) project, PoSICRC2025, 1078 (2025), arXiv:2507.04382 [astro-ph.IM]

    K. Koteraet al.(BEACON and GRAND Collabora- tions), The Hybrid Elevated Radio Observatory for Neu- trinos (HERON) project, PoSICRC2025, 1078 (2025), arXiv:2507.04382 [astro-ph.IM]

  72. [72]

    J. A. Aguilaret al.(RNO-G Collaboration), Design and sensitivity of the Radio Neutrino Observatory in Greenland (RNO-G), JINST16(03), P03025, [Erra- tum: JINST18, E03001(2023)],arXiv:2010.12279[astro- ph.IM]

  73. [73]

    Abarret al.(PUEO Collaboration), The Payload for Ultrahigh Energy Observations (PUEO): a white paper, JINST16(08), P08035, arXiv:2010.02892 [astro-ph.IM]

    Q. Abarret al.(PUEO Collaboration), The Payload for Ultrahigh Energy Observations (PUEO): a white paper, JINST16(08), P08035, arXiv:2010.02892 [astro-ph.IM]

  74. [74]

    Southallet al.(BEACON Collaboration), Searching for RF-only triggered cosmic ray events with the high- elevation BEACON prototype, PoSICRC2021, 1084 (2021)

    D. Southallet al.(BEACON Collaboration), Searching for RF-only triggered cosmic ray events with the high- elevation BEACON prototype, PoSICRC2021, 1084 (2021)

  75. [75]

    Jin, Charm meson induced double cascades in neu- trino telescopes (2024)

    M. Jin, Charm meson induced double cascades in neu- trino telescopes (2024)

  76. [76]

    Abbasiet al.(IceCube Collaboration), Characteriza- tion of the astrophysical diffuse neutrino flux using start- ing track events in IceCube, Phys

    R. Abbasiet al.(IceCube Collaboration), Characteriza- tion of the astrophysical diffuse neutrino flux using start- ing track events in IceCube, Phys. Rev. D110, 022001 (2024), arXiv:2402.18026 [astro-ph.HE]

  77. [77]

    Calculation of conventional and prompt lepton fluxes at very high energy

    A. Fedynitch, R. Engel, T. K. Gaisser, F. Riehn, and T. Stanev, Calculation of conventional and prompt lep- ton fluxes at very high energy, EPJ Web Conf.99, 08001 (2015), arXiv:1503.00544 [hep-ph]

  78. [78]

    The hadronic interaction model SIBYLL 2.3c and Feynman scaling

    F. Riehn, H. P. Dembinski, R. Engel, A. Fedynitch, T. K. Gaisser, and T. Stanev, The hadronic interaction model SIBYLL 2.3c and Feynman scaling, PoSICRC2017, 301 (2018), arXiv:1709.07227 [hep-ph]

  79. [79]

    T. K. Gaisser, T. Stanev, and S. Tilav, Cosmic ray rnergy spectrum from measurements of air showers, Front. Phys. (Beijing)8, 748 (2013), arXiv:1303.3565 [astro-ph.HE]

  80. [80]

    M. G. Aartsenet al.(IceCube Collaboration), Mea- surements using the inelasticity distribution of multi- TeV neutrino interactions in IceCube, Phys. Rev. D99, 032004 (2019), arXiv:1808.07629 [hep-ex]

Showing first 80 references.