Reinterpretation of ATLAS and CMS searches in monojet and mono-V final states: prospects of limits on excited neutrinos
Pith reviewed 2026-06-25 23:34 UTC · model grok-4.3
The pith
Reinterpreting ATLAS and CMS monojet and mono-V searches sets limits on excited-neutrino masses up to 4 TeV.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
By feeding simulated excited-neutrino events into the published ATLAS and CMS monojet and mono-V selections at 13 TeV, the paper obtains cross-section limits that exclude excited-neutrino masses up to approximately 4 TeV for representative benchmark scenarios from the monojet channel; the mono-V channel supplies complementary constraints on the portion of parameter space with large couplings to Standard Model electroweak bosons and low excited-neutrino masses relative to the compositeness scale.
What carries the argument
Reinterpretation of published monojet and mono-V signal regions using simulated excited-neutrino signals to derive mass-dependent cross-section limits.
If this is right
- Monojet searches alone exclude excited-neutrino masses up to approximately 4 TeV in representative benchmark scenarios.
- Mono-V searches constrain the complementary region of large couplings to electroweak bosons and low excited-neutrino masses relative to the compositeness scale.
- The limits are obtained directly from published selections, post-fit backgrounds, and observed yields without requiring new experimental data.
- The approach demonstrates that existing missing-momentum searches already probe a wide class of beyond-Standard-Model scenarios involving excited fermions.
Where Pith is reading between the lines
- Similar reinterpretations could be performed for other composite-fermion models using the same public signal regions.
- Dedicated analyses optimized for the mono-V topology might extend sensitivity at lower masses where the current limits are weaker.
- If the compositeness scale lies close to the excited-neutrino mass, the relative importance of the mono-V channel would increase.
Load-bearing premise
The simulated excited-neutrino signal samples accurately reproduce the kinematics, acceptance, and efficiency in the published ATLAS and CMS signal regions.
What would settle it
An excess of events in the monojet or mono-V signal regions that exceeds the upper limit on the excited-neutrino cross section derived from the simulation would falsify the reported exclusions.
read the original abstract
Searches for final states with large missing transverse momentum recoiling against a jet or a hadronically decaying vector boson provide strong constraints on a wide class of physics scenarios beyond the Standard Model. In this work, we reinterpret existing ATLAS and CMS monojet and mono-$V$ searches at $\sqrt{s} =$ 13 TeV in the context of excited-neutrino production. Published signal-region selections, post-fit background estimates, and observed event yields are used with simulated excited-neutrino signals to derive upper limits on the production cross-section as a function of the excited-neutrino mass. The monojet searches allow excited-neutrino masses of up to approximately 4 TeV to be excluded for representative benchmark scenarios. Mono-$V$ searches provide constraints on the parameter space region with large couplings to the SM electroweak gauge bosons and low excited-neutrino masses compared to the compositeness scale. This is complementary to the region probed by the monojet searches.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reinterprets published ATLAS and CMS monojet and mono-V searches at √s=13 TeV for excited-neutrino production. Published signal-region selections, post-fit background estimates, and observed yields are combined with privately simulated excited-neutrino signal samples to derive upper limits on the production cross section versus excited-neutrino mass. The central claim is that monojet searches exclude masses up to approximately 4 TeV for representative benchmark scenarios, while mono-V searches provide complementary constraints at lower masses and larger electroweak couplings.
Significance. If the simulation accurately reproduces kinematics and efficiencies, the work supplies new, model-specific exclusion limits on excited neutrinos that extend the mass reach of existing data and occupy a complementary region of parameter space. The reuse of published experimental results and yields is a clear strength, enabling reproducible reinterpretation without new experimental effort.
major comments (1)
- [signal simulation and event selection] The 4 TeV mass exclusion in the monojet channel (abstract) is obtained by applying published selections to simulated signal events. No validation of the generator, parton shower, or detector response against published signal efficiencies or control-region closure is described, so the systematic uncertainty on acceptance/efficiency—and therefore on the quoted mass reach—remains unquantified. This assumption is load-bearing for the strongest claim.
Simulated Author's Rebuttal
We thank the referee for the detailed review and for identifying a key point regarding the robustness of our signal simulation. We address the major comment below and will incorporate revisions to strengthen the presentation of uncertainties.
read point-by-point responses
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Referee: [signal simulation and event selection] The 4 TeV mass exclusion in the monojet channel (abstract) is obtained by applying published selections to simulated signal events. No validation of the generator, parton shower, or detector response against published signal efficiencies or control-region closure is described, so the systematic uncertainty on acceptance/efficiency—and therefore on the quoted mass reach—remains unquantified. This assumption is load-bearing for the strongest claim.
Authors: We agree that the manuscript would benefit from an explicit discussion of simulation-related uncertainties. The excited-neutrino signal samples were generated with standard tools (MadGraph5_aMC@NLO + Pythia 8 + Delphes) and the published signal-region selections were applied directly; no dedicated validation against published efficiencies was performed because the original ATLAS/CMS analyses target different BSM models (e.g., dark matter or large extra dimensions) and therefore do not provide signal efficiencies for excited neutrinos. Control-region closure tests in the experimental papers apply to backgrounds, not to our signal. To address the concern we will add a dedicated subsection that (i) describes the generator settings, (ii) reports the effect of reasonable variations in parton-shower and matching parameters on the acceptance, and (iii) assigns a conservative systematic uncertainty to the quoted mass reach. These additions will be included in the revised manuscript. revision: yes
Circularity Check
No circularity detected in derivation chain
full rationale
The paper derives upper limits on excited-neutrino production cross sections by taking published ATLAS/CMS signal-region selections, post-fit background estimates, and observed yields as fixed external inputs and applying them to privately generated signal Monte Carlo samples. No equation, limit, or mass reach reduces by construction to a parameter fitted inside the paper, no result is renamed as a prediction of itself, and no load-bearing premise rests on a self-citation chain. The simulation accuracy assumption is an external modeling choice, not a self-definitional loop, so the central claim remains independent of the paper's own fitted quantities.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
ATLAS Collaboration,Search for new phenomena in events with an energetic jet and missing transverse momentum inppcollisions at √s= 13TeV with the ATLAS detector, Phys. Rev. D103(2021) 112006 [2102.10874]
arXiv 2021
-
[2]
CMS Collaboration,Search for new particles in events with energetic jets and large missing transverse momentum in proton–proton collisions at √s= 13TeV,JHEP11(2021) 153 [2107.13021]
arXiv 2021
-
[3]
Golfand and E.P
Y.A. Golfand and E.P. Likhtman,Extension of the Algebra of Poincare Group Generators and Violation of p Invariance,JETP Lett.13(1971) 323
1971
-
[4]
N. Arkani-Hamed, S. Dimopoulos and G.R. Dvali,The Hierarchy problem and new dimensions at a millimeter,Phys. Lett. B429(1998) 263 [hep-ph/9803315]
Pith/arXiv arXiv 1998
-
[5]
Steigman and M.S
G. Steigman and M.S. Turner,Cosmological Constraints on the Properties of Weakly Interacting Massive Particles,Nucl. Phys. B253(1985) 375
1985
-
[6]
Mimasu, Ken and Sanz, Ver´ onica,ALPs at colliders,JHEP06(2015) 173 [1409.4792]
Pith/arXiv arXiv 2015
-
[7]
Terazawa,Subquark model of leptons and quarks,Phys
H. Terazawa,Subquark model of leptons and quarks,Phys. Rev. D22(1980) 184
1980
-
[8]
Harari,A schematic model of quarks and leptons,Phys
H. Harari,A schematic model of quarks and leptons,Phys. Lett. B86(1979) 83. – 11 –
1979
-
[9]
Fritzsch and G
H. Fritzsch and G. Mandelbaum,Weak interactions as manifestations of the substructure of leptons and quarks,Phys. Lett. B102(1981) 319
1981
-
[10]
U. Baur, M. Spira and P.M. Zerwas,Excited-quark and -lepton production at hadron colliders,Phys. Rev. D42(1990) 815
1990
-
[11]
L3 Collaboration,Search for excited leptons at LEP,Phys. Lett. B568(2003) 23 [hep-ex/0306016]
Pith/arXiv arXiv 2003
-
[12]
OPAL Collaboration,Search for charged excited leptons in e+e- collisions at√s= 183−209GeV,Phys. Lett. B544(2002) 57
2002
-
[13]
DELPHI Collaboration,Search for excited leptons in e+e- collisions at √s= 189−209GeV, Eur. Phys. J. C46(2006) 277 [hep-ex/0603045]
Pith/arXiv arXiv 2006
-
[14]
DELPHI Collaboration,Search for composite and exotic fermions at LEP 2,Eur. Phys. J. C 8(1999) 41 [hep-ex/9811005]
Pith/arXiv arXiv 1999
-
[15]
ALEPH Collaboration,Search for evidence of compositeness at LEP I,Eur. Phys. J. C4 (1998) 571
1998
-
[16]
Chekanov, M
S. Chekanov, M. Derrick, D. Krakauer, S. Magill, B. Musgrave, A. Pellegrino et al.,Searches for excited fermions in ep collisions at HERA,Phys. Lett. B549(2002) 32
2002
-
[17]
Aaron, C
F. Aaron, C. Alexa, V. Andreev, B. Antunovic, S. Aplin, A. Asmone et al.,A search for excited neutrinos ine −pcollisions at HERA,Phys. Lett. B663(2008) 382
2008
-
[18]
Aaron, C
F. Aaron, C. Alexa, K. Alimujiang, V. Andreev, B. Antunovic, A. Asmone et al.,Search for excited quarks in ep collisions at HERA,Phys. Lett. B678(2009) 335
2009
-
[19]
D. Toback and L. ˇZivkovi´ c,Review of Physics Results from the Tevatron: Searches for New Particles and Interactions,Int. J. Mod. Phys. A30(2015) 1541007 [1409.4910]
Pith/arXiv arXiv 2015
-
[20]
ATLAS Collaboration,Search for the production of single vector-like and excited quarks in theW tfinal state inppcollisions at √s= 8TeV with the ATLAS detector,JHEP02(2016) 110 [1510.02664]
Pith/arXiv arXiv 2016
-
[21]
ATLAS Collaboration,Search for new phenomena in dijet events using37fb −1 ofppcollision data collected at √s= 13TeV with the ATLAS detector,Phys. Rev. D96(2017) 052004 [1703.09127]
Pith/arXiv arXiv 2017
-
[22]
ATLAS Collaboration,Search for resonances in the mass distribution of jet pairs with one or two jets identified asb-jets in proton–proton collisions at √s= 13TeV with the ATLAS detector,Phys. Rev. D98(2018) 032016 [1805.09299]
Pith/arXiv arXiv 2018
-
[23]
ATLAS Collaboration,Search for new phenomena in the dijet mass distribution usingpp collision data at √s= 8TeV with the ATLAS detector,Phys. Rev. D91(2015) 052007 [1407.1376]
Pith/arXiv arXiv 2015
-
[24]
ATLAS Collaboration,Search for singleb ∗-quark production with the ATLAS detector at√s= 7TeV,Phys. Lett. B721(2013) 171 [1301.1583]
Pith/arXiv arXiv 2013
-
[25]
ATLAS Collaboration,Search for new phenomena in dijet mass and angular distributions fromppcollisions at √s= 13TeV with the ATLAS detector,Phys. Lett. B754(2016) 302 [1512.01530]
Pith/arXiv arXiv 2016
-
[26]
CMS Collaboration,Search for pair production of excited top quarks in the lepton+jets final state,JHEP06(2014) 125 [1311.5357]. – 12 –
Pith/arXiv arXiv 2014
-
[27]
CMS Collaboration,Search for excited quarks in theγ+jet final state in proton–proton collisions at √s= 8TeV,Phys. Lett. B738(2014) 274 [1406.5171]
Pith/arXiv arXiv 2014
-
[28]
CMS Collaboration,Search for the production of an excited bottom quark decaying totWin proton–proton collisions at √s= 8TeV,JHEP01(2016) 166 [1509.08141]
Pith/arXiv arXiv 2016
-
[29]
CMS Collaboration,Search for excited quarks of light and heavy flavor inγ+ jet final states in proton–proton collisions at √s= 13TeV,Phys. Lett. B781(2018) 390 [1711.04652]
Pith/arXiv arXiv 2018
-
[30]
CMS Collaboration,Search for dijet resonances with data scouting in proton–proton collisions at √s= 13TeV,2510.21641
-
[31]
ATLAS Collaboration,Search for excited leptons in proton–proton collisions at √s= 7TeV with the ATLAS detector,Phys. Rev. D85(2012) 072003 [1201.3293]
Pith/arXiv arXiv 2012
-
[32]
Phys.15(2013) 093011 [1308.1364]
ATLAS Collaboration,Search for excited electrons and muons in √s= 8TeV proton–proton collisions with the ATLAS detector,New J. Phys.15(2013) 093011 [1308.1364]
Pith/arXiv arXiv 2013
-
[33]
Phys.18(2016) 073021 [1601.05627]
ATLAS Collaboration,A search for an excited muon decaying to a muon and two jets inpp collisions at √s= 8TeV with the ATLAS detector,New J. Phys.18(2016) 073021 [1601.05627]
arXiv 2016
-
[34]
ATLAS Collaboration,Search for excited electrons singly produced in proton–proton collisions at √s= 13TeV with the ATLAS experiment at the LHC,Eur. Phys. J. C79 (2019) 803 [1906.03204]
arXiv 2019
-
[35]
ATLAS Collaboration,Search for excitedτ-leptons and leptoquarks in the final state with τ-leptons and jets inppcollisions at √s= 13TeV with the ATLAS detector,JHEP06 (2023) 199 [2303.09444]
arXiv 2023
-
[36]
CMS Collaboration,A search for excited leptons inppcollisions at √s= 7TeV,Phys. Lett. B704(2011) 143 [1107.1773]
Pith/arXiv arXiv 2011
-
[37]
CMS Collaboration,Search for excited leptons inppcollisions at √s= 7TeV,Phys. Lett. B 720(2013) 309 [1210.2422]
Pith/arXiv arXiv 2013
-
[38]
CMS Collaboration,Search for excited leptons in proton–proton collisions at √s= 8TeV, JHEP03(2016) 125 [1511.01407]
Pith/arXiv arXiv 2016
-
[39]
CMS Collaboration,Search for excited leptons inℓℓγfinal states in proton–proton collisions at √s= 13TeV,JHEP04(2019) 015 [1811.03052]
Pith/arXiv arXiv 2019
-
[40]
CMS Collaboration,Search for excited tau leptons in theτ τ γfinal state in proton–proton collisions at √s= 13TeV,JHEP06(2024) 006 [2410.21137]
arXiv 2024
-
[41]
Caliskan,Excited neutrino search potential of the fcc-based electron-hadron colliders,Adv
A. Caliskan,Excited neutrino search potential of the fcc-based electron-hadron colliders,Adv. High Energy Phys.2017(2017) 4726050 [1706.09797]
Pith/arXiv arXiv 2017
-
[42]
A. Caliskan and S.O. Kara,Single production of the excited electrons in the future fcc-based lepton–hadron colliders,Int. J. Mod. Phys. A33(2018) 1850141 [1806.02037]
Pith/arXiv arXiv 2018
-
[43]
ATLAS Collaboration,Search for new phenomena in events with three or more charged leptons inppcollisions at √s= 8TeV with the ATLAS detector,JHEP08(2015) 138 [1411.2921]
Pith/arXiv arXiv 2015
-
[44]
C. Bierlich, S. Chakraborty, N. Desai, L. Gellersen, I. Helenius, P. Ilten et al.,A comprehensive guide to the physics and usage of PYTHIA 8.3,SciPost Phys. Codeb.(2022) [2203.11601]. – 13 –
Pith/arXiv arXiv 2022
-
[45]
DELPHES 3 Collaboration,DELPHES 3: a modular framework for fast simulation of a generic collider experiment,JHEP02(2014) 057 [1307.6346]
Pith/arXiv arXiv 2014
-
[46]
M. Cacciari, G.P. Salam and G. Soyez,The anti-k t jet clustering algorithm,JHEP04(2008) 063 [0802.1189]
Pith/arXiv arXiv 2008
-
[47]
Brun and F
R. Brun and F. Rademakers,Root – an object oriented data analysis framework,Nucl. Instrum. Meth. A389(1997) 81
1997
-
[48]
Garelli, Nicoletta,Performance of the ATLAS Detector in Run-2,EPJ Web Conf.164 (2017) 01021
2017
-
[49]
ATLAS Collaboration,Search for new phenomena in events with an energetic jet and missing transverse momentum inppcollisions at √s= 13TeV with the ATLAS detector, HEPData (collection)(2025)
2025
-
[50]
G. Cowan, K. Cranmer, E. Gross and O. Vitells,Asymptotic formulae for likelihood-based tests of new physics,Eur. Phys. J. C71(2011) 1554 [1007.1727]
Pith/arXiv arXiv 2011
-
[51]
Junk,Confidence level computation for combining searches with small statistics,Nucl
T. Junk,Confidence level computation for combining searches with small statistics,Nucl. Instrum. Meth. A434(1999) 435 [hep-ex/9902006]
Pith/arXiv arXiv 1999
-
[52]
Read,Presentation of search results: theCL s technique,J
A.L. Read,Presentation of search results: theCL s technique,J. Phys. G28(2002) 2693
2002
-
[53]
M. Baak, G. Besjes, D. Cˆ ot´ e, A. Koutsman, J. Lorenz and D. Short,HistFitter software framework for statistical data analysis,Eur. Phys. J. C75(2015) 153 [1410.1280]. [54]CMScollaboration,Overview of the CMS Detector Performance at LHC Run 2,Universe5 (2019) 18
Pith/arXiv arXiv 2015
-
[54]
CMS Collaboration,Identification of heavy, energetic, hadronically decaying particles using machine-learning techniques,JINST15(2020) P06005 [2004.08262]
arXiv 2020
-
[55]
M. Dasgupta, A. Fregoso, S. Marzani and G.P. Salam,Towards an understanding of jet substructure,JHEP09(2013) 029 [1307.0007]
Pith/arXiv arXiv 2013
-
[56]
J.M. Butterworth, A.R. Davison, M. Rubin and G.P. Salam,Jet substructure as a new higgs-search channel at the large hadron collider,Phys. Rev. Lett.100(2008) 242001 [0802.2470]
Pith/arXiv arXiv 2008
-
[57]
CMS Collaboration,Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at √s=13 TeV,HEPData (collection) (2022)
2022
-
[58]
CMS Collaboration,Simplified likelihood for the re-interpretation of public CMS results, CERN-CMS-NOTE-2017-001(2017)
2017
-
[59]
Dembinski, P
H. Dembinski, P. Ongmongkolkul et al.,scikit-hep/iminuit,Zenodo(2020)
2020
-
[60]
James and M
F. James and M. Roos,Minuit: A System for Function Minimization and Analysis of the Parameter Errors and Correlations,Comput. Phys. Commun.10(1975) 343
1975
-
[61]
Karkosova Martinovicova and V
G. Karkosova Martinovicova and V. Pleskot,Reinterpretation of ATLAS and CMS mono-jet and mono-Vsearches in terms of excited neutrinos: public figures,GitLab Repository, https://gitlab.mff.cuni.cz/martinog/excnu_reinterpretation(2026) . – 14 –
2026
discussion (0)
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