Pith.

High Energy Physics - Experiment · arXiv:2609.00842 v1 · submitted 1 Sep 2026 · 56 references

Neutrino Experiments at the LHC and the HL-LHC

Chayanit Asawatangtrakuldee, Albert De Roeck

The paper says

“High energy neutrinos are copiously produced in proton-proton collisions at the Large Hadron Collider (LHC), located at CERN, near Geneva, Switzerland. In particular, a large neutrino flux is expected in the far-forward direction.”

more of the abstract

This flux is concentrated near the beam axis, reaches energies up to the TeV scale, and for electron and tau neutrinos can be dominated by heavy flavour decays at the highest energies. These features open a new experimental window for studying neutrino interactions with dedicated forward detectors, in an energy range beyond the reach of traditional accelerator-based neutrino experiments. The new FASER and SND@LHC experiments reported the first direct observations of neutrino interactions at a hadron collider using the first data from Run 3, which started in 2022. Since then, the programme has advanced to the first measurements, including charged-current neutrino-nucleon cross sections and the detection of different neutrino flavours. This article describes the forward neutrino flux at the LHC, the acceptance and detector concepts of the Run 3 experiments, and summarises the current status of collider neutrino measurements. It also discusses prospects for extending this neutrino programme towards the HL-LHC era. The collected data will also provide constraints on very forward hadron production, and enable searches for feebly interacting particles.

from the abstract

Pith says

Machine review · deepseek-v4-flash · 9 Sep 2026 · what was read was not recorded · not checked by a person

It can be wrong. Challenge this review or reply to it.

No verdict was given on this paper.

2 major objections · 6 minor

How often objections from reviews like this one are right: not yet measured

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Not checked: figures, code, what the 56 references say.

The paper says, at §5, Tables 1 and 2

The review did not quote this passage.

Pith says: Objection 1 of 2 · major

The predicted event rates for Run 3 and HL-LHC are quoted as single numbers without uncertainty bands. Given the discussion in §2.3 that forward charm production uncertainties can be as large as 50% and that different models give spreads in predicted fluxes, the tables should include representative uncertainties or a note in the caption indicating the range from different models.

more of objection 1

Table 1 says 'based on the flux and generator assumptions used in the SND@LHC study [65]' without specifying which model; a brief reference (e.g., 'DPMJET-III/POWHEG predictions') would improve reproducibility.

The paper says, at §4.4

The review did not quote this passage.

Pith says: Objection 2 of 2 · major

Several results are cited from CERN technical notes and conference presentations (Refs [57,58,59,60,61,62,63,64]). The text does label these as 'preliminary' in places, but for a journal review it would be clearer to add an explicit introductory sentence at the start of §4.4 stating that the results in this subsection are preliminary and have not yet undergone journal peer review, to reinforce the distinction from the published results in §§4.1–4.3.

6 minor objections

The paper says, at Abstract

Pith says: minor objection 1 of 6

Hyphenate 'High energy neutrinos' to 'High-energy neutrinos' for consistency.

The paper says, at Figure 7 caption and axes

Pith says: minor objection 2 of 6

The axis labels in the figure should be checked for legibility in print. 'σ/E_ν per nucleon' is clear, but ensure the energy axis has explicit units (GeV).

show 4 more

The paper says, at §2.3, first mention of ξ_w

Pith says: minor objection 3 of 6

The modified scaling variable ξ_w is introduced without definition; define it on first use (e.g., 'the Bodek–Yang model introduces a modified scaling variable ξ_w together with phenomenological K-factors').

The paper says, at §4.2, cross-section values

Pith says: minor objection 4 of 6

The units '(1.2 +0.8/-0.7) × 10^{-38} cm^2 GeV^{-1}' should be written as cm^2/GeV or cm^2 GeV^{-1} consistently; the current notation is slightly ambiguous. Suggest cm^2/GeV.

The paper says, at §5.1, SND@HL-LHC approval

Pith says: minor objection 5 of 6

The text says 'The technical proposal has been approved' (Ref [72]), but it would be helpful to add the approving body (e.g., CERN LHCC) and the month/year of approval for completeness.

The paper says, at References

Pith says: minor objection 6 of 6

Several references are to CERN technical notes and conference proceedings (e.g., [57-64], [65]). For long-term accessibility, consider preferring arXiv e-prints or published proceedings when available. If none exist, add a note that these are 'CERN internal notes or conference presentations'.

What would settle it

Propagate the Sec 2.3 charm QCD scale uncertainty into the Table 1 and Table 2 predicted yields by reweighting the charm-decay component with factorisation and renormalisation scale variations and the POWHEG/DPMJET model spread, then compare the resulting nu_e and nu_tau rates with the un-banded entries. If they move outside a factor of two, the HL-LHC yield tables should carry explicit uncertainty bands and the Sec 4.2 'consistent with SM' cross-section statement should be labeled flux-model dependent.

from the skeptic's reading

How the review went

4 readings by deepseek-v4-flash · 9 Sep 2026

  1. Reader no verdict given confidence moderate
  2. Skeptic partly agrees 1 min 3 s · 23,963 tokens read, 6,652 written
  3. Editor wrote the review in brief 13 s · 24,868 tokens read, 1,143 written
  4. Referee minor revision: 2 major objections, 6 minor 26 s · 24,097 tokens read, 2,752 written

Not run on this paper: the simulated authors' defence.

Pith did not check this review's objections against the paper.

The review in full

The review in brief, machine-written

This is a competent and accurate topical review of the LHC neutrino program through mid-2026. It reliably transmits the published Run 3 results from FASER and SND@LHC—I spot-checked the key numbers and they match the cited papers. The description of forward hadron production uncertainties in Sec 2.3 is honest and well laid out. The review gives a clear, useful overview for anyone new to the field.

The novelty is minimal. This is an explicit update of Ref [21] (Ariga et al., 2025), with one of the same co-authors. The new material is a compilation of 2024–2026 preliminary results from conference talks and CERN technical notes, plus a summary of HL-LHC upgrade concepts. The paper does not claim any new result—it is firmly a review.

The main soft spot: several results in Sec 4.4 (FASER's electronic-detector nu_e observation at 5.5 sigma, SND@LHC's updated zero-muon sample, etc.) come from conference talks and CERN notes that have not completed journal peer review. The review labels them as preliminary, which is appropriate, but a reader should check the final publications when they appear. A second concern: Tables 1 and 2 give predicted event yields with no uncertainties, despite Sec 2.3 quoting charm QCD scale uncertainties up to 50%. The authors could have added a footnote or a reference to the full study. This is a minor omission, not a fatal flaw.

The stress-test note correctly observes that the central claim—that Run 3 established collider neutrinos as detectable—rests on counting-experiment significances computed against expected background, not against forward-flux predictions. Those significances are robust. So the review's main conclusion holds up.

Who is this for? A graduate student or a colleague outside the field who wants a single up-to-date summary of where LHC neutrino physics stands. An expert will already know the published results but might find the compilation of recent preliminary numbers handy for reference.

I would accept peer review. This is a well-executed review that does what it sets out to do. The editor should treat it as a review article, not a research paper, and judge it on clarity, completeness, and accuracy rather than novelty.

The strongest objection

The central assertion - that Run 3 established collider neutrinos as detectable at the LHC - is supported by counting-experiment observations whose significances are computed against expected background, not against forward-flux predictions. FASER's 153+12-13 nu_mu CC candidates (16 sigma, Ref [17]), SND@LHC's 8 events over 0.086 expected background (~7 sigma, Ref [18]), and the nu_0mu sample (9 events over 0.32 background, 6.4 sigma, Ref [56]) stand even if forward charm production is mis-modeled. The Sec 2.3 forward-hadron modeling limitation is real and correctly identified as the dominant systematic for flux normalization: it feeds the 'consistent with Standard Model' cross-section comparisons in Sec 4.2 and leaves Tables 1-2 without explicit uncertainty bands despite the quoted charm QCD scale uncertainties. But the review flags this explicitly, and the HL-LHC program is itself intended to constrain that flux, so the caveat is contained rather than load-bearing for the historical claim. The only residual risk is that the newest Sec 4.4 results cite CERN technical notes and 2026 conference talks not yet through journal review; the review labels these as preliminary, which is appropriate for a status report. No internal inconsistency or unsupported new claim was found.

I read the manuscript as a topical review whose factual spine is the first-observation and first-measurement results from FASER and SND@LHC. I checked the quoted yields and significances against the cited publications as far as possible; they match. The observations are background-limited counting measurements, so they do not depend on forward-hadron modeling; the flux enters only when converting event counts into cross sections or projecting HL-LHC yields. The review itself, in Sec 2.3, identifies forward charm production as the dominant uncertainty for quantitative interpretations, and the reader's weakest_assumption points at the correct systematic. However, the central historical claim - that collider neutrinos can be detected and studied at a hadron collider - would stand even if the charm flux were off by a factor of two, because the detections are established by background rejection and their role as a precision program is explicitly conditional on future flux constraints. The prospects sections are advocacy by program participants, but the central factual claims are independently published, and the review does not present a new physical result. I therefore find no load-bearing defect in the argument; UNVERDICTED for a non-research review remains appropriate and no verdict adjustment is needed.

The referee's report

The review provides a timely and comprehensive snapshot of a rapidly evolving field. If the reported results hold, the LHC is firmly established as a source of multi-TeV neutrinos, enabling a precision programme at the HL-LHC. The paper collects published, peer-reviewed counting-experiment observations whose significances are computed against expected background, not against forward-flux predictions, so the central claim is robust even if the flux modelling uncertainties (discussed in §2.3) are large. The review correctly identifies the forward hadron production modelling as the dominant systematic for flux normalization and cross-section comparisons, and it references the ongoing efforts to constrain it. As a review article, it does not present new original results, but it updates Ref. [21] and includes the most recent preliminary results from 2026 conferences, with appropriate caveats. It will serve as a useful reference for the collider neutrino community.

Pith's reading of the paper (a machine's summary, not the authors')

This review asserts that collider neutrino physics has moved from concept to reality. During LHC Run 3, the FASER and SND@LHC experiments obtained the first direct observations of neutrino interactions at a hadron collider, at energies up to several TeV. These measurements include the first TeV-scale neutrino–nucleon cross sections and the detection of multiple neutrino flavors. The paper argues that these results establish the LHC as a source of high-energy neutrinos and pave the way for a precision program at the HL-LHC, with upgrades already approved. The central implication is that the far-forward region at the LHC has become a laboratory for neutrino physics, QCD, and beyond-the-Standard-Model searches.

What carries the argument. The key machinery is the forward neutrino flux produced in pp collisions at the LHC: collimated near the beam axis and dominated at high energies by decays of charm and bottom hadrons. Dedicated detectors placed ~480 m downstream of the ATLAS interaction point — FASER on the collision axis and SND@LHC off-axis — intercept this flux using dense tungsten targets with nuclear emulsion for micron-scale vertex reconstruction, backed by electronic spectrometers, calorimeters, and muon identification. The on-axis and off-axis configurations provide complementary acceptance and handle the dominant muon-induced backgrounds.

Core claim. The central discovery reviewed is that neutrino interactions can be cleanly observed and studied in the forward direction at the LHC, despite the challenging hadron-collider environment. The first direct observation of collider neutrinos was reported by FASER (153+12−13 νμ CC candidate events, 16σ) and SND@LHC (8 events, 0.086 expected background, ∼7σ). Subsequently, the first TeV-energy-range νe and νμ charged-current cross sections were measured by FASERν, consistent with Standard Model predictions. SND@LHC further observed neutrino interactions without a final-state muon (6.4σ), opening access to NC and νe channels. These results collectively demonstrate that the LHC forward region provides a viable and rich neutrino source for future precision studies.

The premise it rests on. The load-bearing premise is that the forward neutrino flux can be reliably predicted from hadron production models, especially for charm hadrons at large rapidity, where QCD scale uncertainties reach ~50% and can shift the absolute normalization of all extracted cross sections.

If the paper is right (Pith's inferences, not the authors')

The HL-LHC will yield large neutrino samples (e.g., ~10⁴ νμ CC events in upgraded detectors), enabling differential cross sections, flavor ratios, and antineutrino separation.

Collider neutrino data will constrain forward hadron production models — especially charm production — which directly impact predictions for atmospheric neutrino backgrounds in IceCube and KM3NeT.

The experiments serve as dual-purpose platforms: they also search for light, feebly interacting particles (dark photons, axion-like particles, heavy neutral leptons) with world-leading sensitivity.

ντ interactions, otherwise difficult to study, become accessible via the charm-decay flux, allowing tests of lepton flavor universality at TeV energies.

Cross-section measurements at TeV energies provide benchmarks for high-energy astrophysical neutrino detectors and for future collider facilities (FCC, muon collider).

If forward charm production uncertainties (quoted at up to ~50% for scale variations) are not reduced by dedicated measurements like DsTau/NA65, the absolute flux normalization for νe and ντ will remain the dominant systematic for cross-section extractions in all HL-LHC projections.

The complementarity between on-axis (FASER) and off-axis (SND@LHC) detectors could be exploited to isolate systematic effects from beamline geometry and muon background modeling, strengthening combined flux and cross-section results.

A decision to build the Forward Physics Facility (FPF) would enlarge the program by a factor of 5–20 in event yield and enable detector redundancy; the paper implicitly assumes that the tunnel-based upgrades (FASERν2, SND@HL-LHC) are the baseline for Run 4, but the FPF remains a more ambitious option whose feasibility studies are ongoing.

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The paper

Abstract

High energy neutrinos are copiously produced in proton-proton collisions at the Large Hadron Collider (LHC), located at CERN, near Geneva, Switzerland. In particular, a large neutrino flux is expected in the far-forward direction. This flux is concentrated near the beam axis, reaches energies up to the TeV scale, and for electron and tau neutrinos can be dominated by heavy flavour decays at the highest energies. These features open a new experimental window for studying neutrino interactions with dedicated forward detectors, in an energy range beyond the reach of traditional accelerator-based neutrino experiments. The new FASER and SND@LHC experiments reported the first direct observations of neutrino interactions at a hadron collider using the first data from Run 3, which started in 2022. Since then, the programme has advanced to the first measurements, including charged-current neutrino-nucleon cross sections and the detection of different neutrino flavours. This article describes the forward neutrino flux at the LHC, the acceptance and detector concepts of the Run 3 experiments, and summarises the current status of collider neutrino measurements. It also discusses prospects for extending this neutrino programme towards the HL-LHC era. The collected data will also provide constraints on very forward hadron production, and enable searches for feebly interacting particles.

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. No sentence in this record was written by a model.

abstract compiled · 2026-09-23

The authors' main claim, as the classifier picked it out 0.63

“These features open a new experimental window for studying neutrino interactions with dedicated forward detectors, in an energy range beyond the reach of traditional accelerator-based neutrino experiments.”

How the main claim is stated: asserted 0.75

What the abstract itself states, as probabilities: claims first 0.66 · states limitation 0.10 · human participants 0.03 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.12 · compares with prior results 0.30 · mentions code or data availability 0.02

The abstract, sentence by sentence

This table labels the abstract only (arXiv listing abstract v1). The number is the probability the classifier gave the label.

SentenceRoleThe authors' own workStates the main conclusionStrength
High energy neutrinos are copiously produced in proton-proton collisions at the Large Hadron Collider (LHC), located at CERN, near Geneva, Switzerland. background 1.00 0.09 0.04 asserted 1.00
In particular, a large neutrino flux is expected in the far-forward direction. background 0.95 0.11 0.04 hedged possibility 0.79
This flux is concentrated near the beam axis, reaches energies up to the TeV scale, and for electron and tau neutrinos can be dominated by heavy flavour decays at the highest energies. background 0.97 0.14 0.05 asserted 0.84
These features open a new experimental window for studying neutrino interactions with dedicated forward detectors, in an energy range beyond the reach of traditional accelerator-based neutrino experiments. background 0.43 0.09 0.16 asserted 0.75
The new FASER and SND@LHC experiments reported the first direct observations of neutrino interactions at a hadron collider using the first data from Run 3, which started in 2022. result 0.55 0.28 0.17 asserted 1.00
Since then, the programme has advanced to the first measurements, including charged-current neutrino-nucleon cross sections and the detection of different neutrino flavours. result 0.49 0.29 0.08 asserted 1.00
This article describes the forward neutrino flux at the LHC, the acceptance and detector concepts of the Run 3 experiments, and summarises the current status of collider neutrino measurements. contribution 0.99 0.32 0.09 asserted 0.97
It also discusses prospects for extending this neutrino programme towards the HL-LHC era. future work 0.85 0.28 0.07 asserted 0.84
The collected data will also provide constraints on very forward hadron production, and enable searches for feebly interacting particles. future work 0.56 0.21 0.09 asserted 0.58

What kind of paper the classifier reports this is: review 0.91 · evidence from observation or experiment 0.52

What was examined, and what was not

Sources read

  • arXiv listing abstract v1

Not examined

  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers

Levels run

  • P abstract

Not run

  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

How the labels were made

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,954 input tokens.

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. This record as JSON

Figures (17)
Figure 1 of the paper
Figure 1. Expected LHC luminosity profile, updated by the authors to reflect the LHC schedule as of April 2026. Adapted from Ref. [20] (CC BY 4.0). recording neutrino interactions, in particular because of the good ντ identification potential of such a detector. The LHC Run 3 started in 2022, at a time by which the landscape had considerably developed. By then, two new experiments in the forward region, FASER and SND@LHC, had been proposed, approved, and installed, and were ready to take data when pp collisions resumed at the LHC. Both experiments very quickly reported the first direct…
Figure 2 of the paper
Figure 2. Layout of the forward experiments around the ATLAS detector at the LHC. Adapted from Ref. [21] (CC BY 4.0)
Figure 3 of the paper
Figure 3. Neutrino distribution in the (η, E) plane, simulated with the PYTHIA 8 program and weighted by the interaction probability. Colors denote neutrinos from W decays, bottom hadrons, charm hadrons, and light hadrons. Adapted from Ref. [26] (CC BY 4.0); insets follow the original. translate into small transverse displacements, r ≃ Lθ. At L ∼ 480 m, a 1 mrad angle corresponds to r ∼ 0.5 m, which is why compact transverse detectors in existing service tunnels can intercept a sizable fraction of the far-forward flux. Since the neutrino energies are typically in the range of a few hundred…
Figure 4 of the paper
Figure 4. Schematic layout of the FASER detector, including the upstream FASERν emulsion target, the decay volume for dark sector particle searches, the magnetic spectrometer with tracking stations, and the electromagnetic calorimeter. Adapted from Ref. [23] (CC BY 4.0). 3.2 SND@LHC experiment SND@LHC (Scattering and Neutrino Detector at the LHC) originated from the merger of ideas developed in the XSEN proposal [15] and in the proposed SND detector for neutrino detection in the SHiP fixed target beam-dump experiment at CERN [52]. At the time, the future of SHiP was still uncertain.…
Figure 5 of the paper
Figure 5. Schematic layout of the SND@LHC detector, including the upstream veto system, the emulsion–tungsten target and vertex detector with scintillating fibre (SciFi) tracking planes, and the downstream hadronic calorimeter and muon identification system. Adapted from Ref. [25] (CC BY 4.0). • FASER: Using 2022 pp data at √ s = 13.6 TeV corresponding to 35.4 fb−1 , FASER identified νµ CC candidates with a penetrating muon reconstructed in the magnetic spectrometer and consistent with an interaction in the upstream target region. A key feature of the FASER strategy was the use of an…
Figure 6 of the paper
Figure 6. Left: distribution of the extrapolated track position at the FASERν scintillator plane, rveto ν, versus the reconstructed muon momentum pµ for the 2022 dataset. The dashed lines indicate the signal region definition used in the FASER νµ CC analysis. Adapted from Refs. [17] (CC BY 4.0). Right: distribution of the number of SciFi hits for the selected sample in the SND@LHC νµ CC analysis, comparing data to the neutrino simulation and to the neutral hadron background estimate. Adapted from Ref. [18] (CC BY 4.0). The measurement combined neutrino and antineutrino interactions, and the…
Figure 7 of the paper
Figure 7. Measured σ/Eν per nucleon for νe (top) and νµ (bottom) in the TeV energy range, compared to the Standard Model predictions. The dashed contours labeled “Bodek–Yang” indicate the Bodek–Yang cross section model used for comparison. Adapted from Ref. [53] (CC BY 4.0)
Figure 8 of the paper
Figure 8. Measured νµ charged-current cross section divided by neutrino energy as a function of neutrino energy, compared to Bodek–Yang predictions and previous neutrino measurements. Adapted from Ref. [54] (CC BY 4.0). 9
Figure 9 of the paper
Figure 9. Distribution of the sum of SciFi hit-density weights used as the main discriminant in the SND@LHC ν0µ analysis, comparing data to the expected signal and background contributions. Adapted from Ref. [56] (CC BY 4.0)
Figure 10 of the paper
Figure 10. A νe and a νµ interaction candidate in the FASER emulsion target. Adapted from Ref. [57]. towards more differential cross section measurements, and first studies of more exclusive neutrino interaction topologies. FASER. FASER has presented updated results on high energy electron and muon neutrino CC interactions in the FASERν emulsion–tungsten sub-detector. A subset of the FASERν volume was used, corresponding to a target mass of 681.1 kg and an exposure of 9.5 fb−1 of LHC pp collision data collected in 2022 [57, 58]. The muon neutrino energy is reconstructed using a regression…
Figure 11 of the paper
Figure 11. Left: measured νµ and νe CC neutrino–nucleon cross sections from the FASERν emulsion detector and the FASER electronic detector, compared with theoretical predictions. Right: post-fit calorimeter electromagnetic energy distribution in the νe signal region, showing an excess of 65 ± 12 events above background. Adapted from Ref. [58]. The preliminary FASER cross section and electronic detector νe results are shown in
Figure 12 of the paper
Figure 12. Distributions of the summed hit-density weights in the target used in the zero muon analysis for (left) test-beam data samples and (right) the 2022–2024 data sample corresponding to an integrated luminosity of 170.6 fb−1 [62]. distributions with the FLUKA-based simulation chain for the different LHC optics and crossing configurations [64]. At a reference instantaneous luminosity of 2 × 1034 cm−2 s −1 , the measured rates were 557, 1154 and 799 Hz for the 2022–2023, 2024 and 2025 configurations, respectively, with simulation and data agreeing at the level of about 10–15%. The…
Figure 13 of the paper
Figure 13. Schematic views of two upgrade concepts discussed for the ATLAS interaction point collider neutrino programme. Left: reference on-axis upgraded FASER neutrino detector concept with an active tungsten target and readout, designed to fit within the TI12/UJ12 tunnel constraints. Right: upgraded SND@HL-LHC concept showing the neutrino target, veto system, and magnetised calorimeter for charge and momentum measurement. Adapted from Refs. [71, 73] (CC BY 4.0). 5.2 Forward Physics Facility concepts The Forward Physics Facility (FPF) is a proposal for a dedicated large far-forward…
Figure 14 of the paper
Figure 14. Site and line of sight sketch for the proposed Forward Physics Facility (FPF) cavern location. Adapted from Ref. [79] (CC BY 4.0). to collect high statistics interaction samples. It targets precision measurements of TeV scale neutrino cross sections and flavour samples, with sensitivity to νe and ντ through high resolution vertexing and lepton identification. • FLArE: a liquid-argon time projection chamber (LArTPC) detector concept that provides a massive target and rich event information for neutrino interactions. LArTPCs are like elec￾tronic “bubble chambers”, giving high quality…
Figure 15 of the paper
Figure 15. 3D view of the surface building, shaft, and underground cavern for the proposed FPF. Adapted from Ref. [79] (CC BY 4.0)
Figure 16 of the paper
Figure 16. Layout of the proposed FPF cavern with the placement of the four detector concepts (FASER2, FASERν2, FLArE, and FORMOSA). Adapted from Ref. [79] (CC BY 4.0). 16
Figure 17 of the paper
Figure 17. Schematic overview of the SINE and UNDINE concepts, showing detector locations on the surface and under the lake, and the corresponding beam geometries. The shaded envelope shown around each beamline corresponds to the profile of the neutrino beam passing through the FASER detector. Adapted from Ref. [81] (CC BY 4.0). ratio [85]. In this case, muons with measured charge provide a handle to separate neutrino and antineutrino contributions. 6 Physics opportunities and outlook The first observation of neutrino interactions at the LHC in Run 3 has opened a new direction for neutrino…

Figures are the authors', reproduced from the paper.

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