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REVIEW 3 major objections 2 minor

First double-differential muon-neutrino charged-current cross section on oxygen versus kinematic imbalance, extracted jointly with carbon and with no pions and at least one proton in the final state.

Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →

T0 review · grok-4.5

2026-07-15 09:12 UTC pith:35SGQOE5

load-bearing objection First joint C–O double-differential KI cross section in CC0π+Np from T2K ND280; useful for nuclear systematics, residual model dependence is the usual structural caveat and cannot be audited from the abstract alone. the 3 major comments →

arxiv 2607.10638 v2 pith:35SGQOE5 submitted 2026-07-12 hep-ex

First double-differential measurement of pionless charged-current muon neutrino interactions using kinematic imbalance observables on carbon and oxygen with the T2K experiment

K. Abe , S. Abe , H. Adhikary , R. Akutsu , H. Alarakia-Charles , Y.I. Alj Hakim , S. Alonso Monsalve , L. Anthony
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S. Aoki K.A. Apte T. Arai T. Arihara S. Arimoto Y. Asami Y. Asaoka Y. Ashida E.T. Atkin N. Babu V. Baranov G.J. Barker G. Barr D. Barrow P. Bates L. Bathe-Peters M. Batkiewicz-Kwasniak N. Baudis V. Berardi L. Berns S. Bhattacharjee A. Blanchet A. Blondel L. B{\o}e P.M.M. Boistier S. Bolognesi S. Bordoni S.B. Boyd C. Bronner A. Bubak M. Buizza Avanzini J.A. Caballero N.F. Calabria D. Calvet S. Cao D. Carabadjac S.L. Cartwright M.P. Casado M.G. Catanesi J. Chakrani A. Chalumeau D. Cherdack A. Chvirova J. Coleman G. Collazuol F. Cormier A.A.L. Craplet A. Cudd D. D'Ago C. Dalmazzone T. Daret C. Davis Yu.I. Davydov P. de Perio G. De Rosa T. Dealtry C. Densham A. Dergacheva R. Dharmapal Banerjee F. Di Lodovico G. Diaz Lopez S. Dolan T.A. Doyle O. Drapier K.E. Duffy J. Dumarchez P. Dunne K. Dygnarowicz M. El Baz J. Elias S. Emery-Schrenk G. Erofeev A. Ershova G. Eurin M. Fani D. Fedorova S. Fedotov M. Feltre L. Feng D. Ferlewicz A.J. Finch M.D. Fitton C. Forza M. Friend Y. Fujii Y. Fukuda N. Funayama A.N. Gaci\~no Olmedo J. Garc\'ia-Marcos A.C. Germer L. Giannessi C. Giganti M. Girgus V. Glagolev M. Gonin R. Gonzalez Jimenez J. Gonz\'alez Rosa K. Gorshanov P. Govindaraj M. Grassi M. Guigue F.Y. Guo D.R. Hadley S. Han D.A. Harris R.J. Harris M. Hartz T. Hasegawa C.M. Hasnip S. Hassani N.C. Hastings K. Hayashi Y. Hayato I. Heitkamp D. Henaff Y. Hino K. Hiraide J. Holeczek A. Holin N.T. Hong Van T. Honjo M.C.F. Hooft R. Huang J. Hu A.K. Ichikawa K. Ieki M. Ikeda T.H. Ishida T. Ishida M. Ishitsuka H. Ito S. Ito A. Izmaylov N. Jachowicz B. Jargowsky S.J. Jenkins C. Jes\'us-Valls J.Y. Ji T.P. Jones P. Jonsson C.K. Jung M. Kabirnezhad A.C. Kaboth K. Kadota H. Kakuno A. Kamata J. Kameda S. Karpova V.S. Kasturi Y. Kataoka T. Katori R. Kawabe M. Kawaue E. Kearns M. Khabibullin N.V. Khomutov A. Khotjantsev T. Kikawa S. King V. Kiseeva J. Kisiel A. Klustov\'a L. Kneale H. Kobayashi S.R. Kobayashi T. Kobayashi L. Koch S. Kodama M. Kolupanova L.L. Kormos Y. Koshio K. Kowalik R. Kralik Y. Kudenko A. Kumar Jha R. Kurjata V. Kurochka T. Kutter L. Labarga M. Lachat K. Lachner J. Lagoda S.M. Lakshmi M. Lamers James A. Langella D.H. Langridge J.-F. Laporte D. Last N. Latham M. Laveder L. Lavitola M. Lawe A. Leclerc N. Lemaire D. Leon Silverio T. Leplumey S. Levorato S.V. Lewis B. Li C. Lin R.P. Litchfield W. Li A. Longhin L. Ludovici X. Lu T. Lux L.N. Machado L. Magaletti K. Mahn K.K. Mahtani S. Manly D.G.R. Martin D.A. Martinez Caicedo L. Martinez M. Martini N. Mashin T. Matsubara R. Matsumoto C. Mauger K. Mavrokoridis N. McCauley K.S. McFarland C. McGrew J. McKean A. Mefodiev G.D. Megias L. Mellet C. Metelko M. Mezzetto S. Miki V. Mikola E.W. Miller A. Minamino O. Mineev S. Mine J. Mirabito M. Miura S. Moriyama P. Morrison Th.A. Mueller D. Munford A. Mu\~noz L. Munteanu Y. Nagai T. Nakadaira K. Nakagiri M. Nakahata Y. Nakajima K.D. Nakamura A. Nakano Y. Nakano S. Nakayama T. Nakaya K. Nakayoshi C.E.R. Naseby D.T. Nguyen V.Q. Nguyen K. Niewczas S. Nishimori Y. Nishimura Y. Noguchi T. Nosek F. Nova J.C. Nugent H.M. O'Keeffe L. O'Sullivan W. Okinaga K. Okumura T. Okusawa N. Onda N. Ospina L. Osu N. Otani Y. Oyama V. Paolone J. Pasternak D. Payne T.P.D. Peacock M. Pfaff L. Pickering J.-B. Plan\c{c}on P. Podlaski B. Popov A.J. Portocarrero Yrey M. Posiadala-Zezula Y.S. Prabhu H. Prasad F. Pupilli B. Quilain P.T. Quyen E. Radicioni M.A. Ramirez Delgado R. Ramsden P.N. Ratoff M. Reh G. Reina L. Restrepo C. Riccio D.W. Riley E. Rondio D. Ross S. Roth N. Roy A. Rubbia L. Russo A. Rychter W. Saenz K. Sakashita S. Samani F. S\'anchez E.M. Sandford Y. Sato T. Schefke K. Scholberg M. Scott Y. Seiya T. Sekiguchi H. Sekiya M. Sekiyama T. Sekiya D. Seppala D. Sgalaberna A. Shaikhiev M. Shiozawa Y. Shiraishi N. Shvarev A. Shvartsman V. Siccardi N. Skrobova K. Skwarczynski D. Smyczek M. Smy J.T. Sobczyk H. Sobel F.J.P. Soler A.J. Speers R. Spina A. Srivastava P. Stowell Y. Stroke I.A. Suslov A. Suzuki M. Suzuki S.Y. Suzuki M. Tada A. Takeda Y. Takeuchi K. Takeya H.K. Tanaka H. Tanigawa A. Teklu V.V. Tereshchenko N. Thamm C. Touramanis N. Tran T. Tsukamoto M. Tzanov M. Vagins M. Varghese I. Vasilyev G. Vasseur E. Villa U. Virginet T. Vladisavljevic T. Wachala H.T. Wallace J.G. Walsh D. Wark M.O. Wascko A. Weber R. Wendell M.J. Wilking C. Wilkinson C. Winterstein C. Wret J. Xia Z. Xie K. Yamamoto T. Yamamoto T. Yamazumi C. Yanagisawa Y. Yang T. Yano N. Yershov U. Yevarouskaya M. Yokoyama Y. Yoshimoto N. Yoshimura A. Zalewska J. Zalipska G. Zarnecki J. Zhang X.Y. Zhao H. Zheng H. Zhong M. Ziembicki M. Zito
This is my paper
classification hep-ex
keywords neutrino–nucleus interactionscharged-current cross sectionkinematic imbalanceoxygen targetcarbon targetT2K ND280pionless final statenuclear effects
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved

The pith

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

This paper reports the first measurement of the muon-neutrino charged-current cross section on oxygen as a function of kinematic-imbalance observables, for events that produce no pions and at least one proton. The T2K ND280 near detector extracts the cross section simultaneously on carbon and oxygen, double-differentially in several imbalance variables. Those variables are sensitive to nuclear effects that redistribute energy and momentum inside the nucleus, effects that currently limit the precision of neutrino-oscillation experiments. Because the two targets are measured together, the result also supplies the C–O correlations needed when an experiment (T2K, Hyper-Kamiokande) uses multiple nuclear targets. None of the widely used neutrino-event generators fully reproduces the measured distributions across the whole phase space, so the data give concrete guidance on where nuclear models must improve.

Core claim

The first double-differential measurement of the pionless, proton-tagged muon-neutrino charged-current cross section on oxygen (and simultaneously on carbon) as a function of kinematic-imbalance observables, obtained with T2K ND280; the joint extraction yields direct experimental sensitivity to carbon–oxygen correlations, and no existing generator describes the data in every region of the measured phase space.

What carries the argument

Kinematic-imbalance (KI) observables—quantities constructed from the measured muon and proton momenta that vanish for a free nucleon at rest—serve as the experimental handles that isolate nuclear effects; the double-differential cross sections in these variables, extracted jointly for carbon and oxygen, are the central results that expose model deficiencies and C–O correlations.

Load-bearing premise

The efficiency corrections and unfolding used to extract the double-differential cross sections are assumed to be free enough of residual nuclear-model dependence that the reported distributions and C–O correlations remain unbiased.

What would settle it

A future measurement of the same pionless, proton-tagged double-differential distributions on oxygen (or carbon) with an independent detector and different efficiency model that yields statistically incompatible shapes in any of the kinematic-imbalance variables would falsify the present extraction.

Watch this falsifier. Get emailed when new claim-graph text bears on it.

If this is right

  • Joint C–O cross sections supply the target-correlation matrix needed to reduce a major systematic in multi-target oscillation analyses such as T2K and Hyper-Kamiokande.
  • Regions of kinematic-imbalance phase space that are poorly described by all generators become priority targets for nuclear-model revision.
  • The pionless, proton-tagged topology isolates final-state interactions and multi-nucleon effects without pion-absorption ambiguities.
  • The same KI framework can be reapplied to other nuclei or to antineutrino beams once statistics allow.

Where Pith is reading between the lines

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

  • If residual model dependence in the ND280 efficiency is later shown to be large, the claimed C–O correlations would have to be re-extracted with a more model-independent technique before they can be used in oscillation fits.
  • The persistent generator discrepancies in high-imbalance tails suggest that current treatments of short-range correlations or final-state re-scattering are incomplete for light nuclei.
  • Extending the identical analysis to argon or water-rich targets would test whether the same nuclear deficiencies scale with mass number.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

3 major / 2 minor

Summary. The manuscript reports the first double-differential measurement of the muon-neutrino charged-current cross section as a function of kinematic-imbalance (KI) observables for the CC0π+Np topology on oxygen, extracted simultaneously with carbon using T2K ND280. The joint C/O extraction is presented as providing direct sensitivity to target correlations relevant for multi-target oscillation analyses (T2K, Hyper-Kamiokande). Generator comparisons are said to show that none of the widely used models fully describe the data across the measured phase space, motivating improvements in nuclear-effect modeling.

Significance. If the extraction is sufficiently free of residual nuclear-model bias, a first joint C/O double-differential KI measurement in the pionless, proton-tagged channel would be a valuable constraint for neutrino-nucleus generators and a concrete input for reducing multi-target systematics in current and next-generation oscillation experiments. The simultaneous-target design and the focus on KI observables are well-motivated. The abstract’s claim that no generator fully describes the data would, if robust, be a useful falsification signal for the community. These strengths cannot be fully assessed from the abstract alone.

major comments (3)
  1. Only the abstract is available for this review, so efficiency corrections, background subtraction, unfolding regularization, flux uncertainties, and the quantitative treatment of C–O correlations cannot be audited. The central claim—that residual model dependence does not bias the reported double-differential KI distributions or the claimed target correlations—is load-bearing and cannot be verified without the full analysis description, covariance treatment, and model-variation studies.
  2. Abstract claim that ‘none of the models fully describe the data across all regions of measured phase space’: without the full text it is impossible to judge how this is quantified (χ², pull distributions, phase-space binning, or visual comparison only). A load-bearing statement of this form requires explicit, reproducible comparison metrics and a clear statement of which phase-space regions drive the disagreement.
  3. Abstract claim of ‘direct sensitivity to the correlations between two targets’: the joint C/O extraction is presented as reducing systematics for multi-target oscillation experiments. The residual model dependence of proton-tagging and pion-veto efficiencies (and of any unfolding of δpT, δφT, etc.) on the same FSI/2p2h generators under test is the principal risk to reading those correlations as genuine constraints. The abstract supplies no quantification of that residual dependence; the full manuscript must demonstrate that the reported C–O correlations are not pulled toward the prior.
minor comments (2)
  1. Abstract: the phrase ‘kinematic imbalance (KI) observables’ is used without naming the specific variables (e.g. δpT, δφT, δpTT). Naming them would improve clarity for non-specialist readers of the abstract.
  2. Abstract: ‘at least one proton in the final state’ should be stated with the proton momentum/threshold definition used in the selection, even at abstract level, since that threshold strongly affects FSI sensitivity.

Circularity Check

0 steps flagged

No significant circularity: data-driven double-differential cross-section measurement compared to external generators.

full rationale

This is an experimental measurement paper (T2K ND280) reporting the first joint carbon/oxygen double-differential charged-current cross sections as a function of kinematic-imbalance observables in the CC0π+Np channel. The abstract presents extracted cross sections and compares them to external neutrino event generators; none of the generators fully describe the data. There is no derivation chain that reduces a claimed first-principles prediction to a fitted input by construction, no uniqueness theorem imported from the authors, no ansatz smuggled via self-citation, and no renaming of a known empirical pattern as a new theoretical result. Residual model dependence in efficiency and unfolding corrections is a standard experimental systematic (correctness/systematics risk), not circularity of the kind defined by the patterns: the reported distributions are not forced by definition to equal the generators under test. With only the abstract available and no equations or self-citation load-bearing steps exhibited, the honest finding is score 0 with empty steps.

Axiom & Free-Parameter Ledger

0 free parameters · 4 axioms · 0 invented entities

Abstract-only experimental measurement. No free parameters are fitted to produce a ‘prediction’; the result is a measured cross section. Background axioms are standard HEP detector and flux assumptions that any ND280 analysis inherits. No new particles or forces are postulated.

axioms (4)
  • domain assumption ND280 detector response, reconstruction efficiency, and particle identification for muons and protons are correctly modeled after calibration.
    Any cross-section extraction on ND280 depends on this; residual mismodeling would bias the reported KI distributions.
  • domain assumption T2K neutrino flux prediction and its uncertainty are adequate for absolute cross-section normalization.
    Absolute CC cross sections inherit flux scale; abstract does not quantify residual flux systematics.
  • domain assumption Selected final state (no pions, ≥1 proton) can be isolated with controllable purity and efficiency.
    The channel definition is load-bearing for the claimed ‘pionless’ measurement.
  • standard math Standard charged-current weak interaction and muon-neutrino beam composition.
    Background particle-physics framework; not under test.

pith-pipeline@v1.1.0-grok45 · 8376 in / 2452 out tokens · 28145 ms · 2026-07-15T09:12:33.364407+00:00 · methodology

0 comments
read the original abstract

We report the first measurement of muon-neutrino charged-current cross section as a function of kinematic imbalance (KI) observables on oxygen with no pions and at least one proton in the final state, using the T2K ND280 detector. The cross section is extracted simultaneously for carbon and oxygen targets and double-differentially as a function of several KI observables, providing new insight into the modeling of nuclear effects. This joint measurement offers direct sensitivity to the correlations between two targets, a key ingredient for reducing systematic uncertainties in neutrino oscillation experiments that employ multiple target nuclei, such as T2K and Hyper-Kamiokande. Comparisons with predictions from widely used neutrino event generators show that none of the models fully describe the data across all regions of measured phase space. These results highlight possible directions where improvements in neutrino-nucleus interaction modeling are needed for current and future neutrino oscillation experiments.

discussion (0)

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