Sensitivity prospects for lepton-trijet signals in the νSMEFT at the LHeC
Pith reviewed 2026-05-24 07:59 UTC · model grok-4.3
The pith
The LHeC can constrain effective couplings of 100-500 GeV heavy neutrinos to order 0.1 at 1 TeV scale via lepton-trijet signals.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The LHeC with 100 fb^{-1} luminosity can probe the scenario of a heavy neutral lepton N in the 100-500 GeV range and constrain the effective couplings in the νSMEFT to a region as tight as the bounds currently considered for O(10) GeV scale masses, with effective couplings of O(10^{-1}) for a new physics scale Λ = 1 TeV, through the lepton flavor violating and lepton number violating lepton-trijet channels.
What carries the argument
Lepton-trijet signals (p e^{-} → μ^{±} + 3 jets) in the νSMEFT, which encode the effective interactions of heavy neutral leptons with standard model fields below the new physics scale.
If this is right
- The LHeC would set competitive limits on electroweak-scale heavy neutrinos that match current constraints for lighter masses.
- Both lepton-flavor-violating and lepton-number-violating channels would be accessible at comparable sensitivity.
- The results would directly test νSMEFT operators involving heavy neutral leptons at a future electron-proton facility.
- No significant degradation of reach is expected from detector effects once standard reconstruction is applied.
Where Pith is reading between the lines
- Clean electron-proton collisions at the LHeC could complement hadron-collider searches by reducing QCD backgrounds in lepton-number-violating channels.
- The quoted sensitivity assumes the new physics scale sits at 1 TeV; higher scales would weaken the bounds proportionally.
- Similar trijet analyses could be repeated at higher luminosity or at other proposed electron-proton machines to map the full viable parameter space.
Load-bearing premise
That the lepton-trijet signals from heavy neutrinos can be isolated from standard model backgrounds at the LHeC using realistic detector simulations without major loss of sensitivity.
What would settle it
A full LHeC detector simulation in which standard model backgrounds in the muon-plus-three-jet channels exceed the expected signal rate for effective couplings of 0.1 across the 100-500 GeV mass window.
read the original abstract
The observation of neutrino oscillations and masses motivates the extension of the standard model with right handed neutrinos, leading to heavy neutrino states possibly in the electroweak scale, which could be impacted by new high-scale weakly coupled physics. A systematic tool for studying these interactions is the neutrino-extended standard model effective field theory $\nu$SMEFT. In this work we study the prospects of the future LHeC electron-proton collider to discover or constrain the $\nu$SMEFT interactions, performing the first dedicated and realistic analysis of the well known lepton-trijet signals, both for the lepton flavor violating $p ~ e^{-} \rightarrow \mu^{-} + 3 \mathrm{j}$ (LFV) and the lepton number violating $p ~ e^{-} \rightarrow \mu^{+} + 3 \mathrm{j}$ (LNV) channels, for HNLs masses in the electroweak scale range: $100 ~\rm GeV \leq m_N \leq 500 ~\rm GeV$. The obtained sensitivity prospects show that the LHeC with $100 ~\rm fb^{-1}$ luminosity could be able to probe the scenario of a heavy $N$ and constrain the effective couplings to a region of the parameter space as tight as the bounds that are currently considered for the $\mathcal{O}(10)$GeV scale masses, with effective couplings of $\mathcal{O}(10^{-1})$ for NP scale $\Lambda=1 \rm TeV$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that the LHeC with 100 fb^{-1} can probe heavy neutral leptons (HNLs) with masses 100-500 GeV via lepton-trijet signals in the νSMEFT, for both LFV (e^{-}p → μ^{-} + 3j) and LNV (e^{-}p → μ^{+} + 3j) channels. It asserts that the resulting constraints on effective couplings reach O(10^{-1}) for Λ=1 TeV, comparable to existing bounds at O(10) GeV masses, based on a first dedicated realistic analysis.
Significance. If substantiated by the underlying simulation and statistical details, the result would extend collider sensitivity to electroweak-scale HNLs in an EFT framework and provide competitive limits on νSMEFT operators at a future ep machine.
major comments (1)
- [Abstract] Abstract: the central sensitivity claim rests on an unspecified 'dedicated and realistic analysis' of lepton-trijet signals, detector simulations, background estimation, and statistical methods, none of which are provided; without these the quoted reach (O(10^{-1}) couplings at Λ=1 TeV) cannot be verified and is therefore load-bearing for the paper's conclusion.
Simulated Author's Rebuttal
We thank the referee for their feedback on our manuscript. We address the major comment below.
read point-by-point responses
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Referee: [Abstract] Abstract: the central sensitivity claim rests on an unspecified 'dedicated and realistic analysis' of lepton-trijet signals, detector simulations, background estimation, and statistical methods, none of which are provided; without these the quoted reach (O(10^{-1}) couplings at Λ=1 TeV) cannot be verified and is therefore load-bearing for the paper's conclusion.
Authors: The abstract provides a concise summary of the results. The full manuscript contains dedicated sections describing the lepton-trijet analysis for both the LFV and LNV channels. These include the Monte Carlo generation of signal and background events, modeling of the LHeC detector response, estimation of Standard Model backgrounds, and the statistical framework used to extract the sensitivity on the effective couplings at Λ=1 TeV. The quoted reach follows directly from this analysis as detailed in the main text. revision: no
Circularity Check
No circularity in available abstract
full rationale
Only the abstract is provided, which describes a forward sensitivity projection for LHeC lepton-trijet signals without any equations, fitted parameters, self-citations, or derivation steps. The central claim rests on an unshown 'dedicated and realistic analysis' of signal isolation, but no load-bearing step reduces by construction to inputs or prior self-work. This is the normal case of a self-contained projection study with no detectable circularity patterns.
discussion (0)
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