pith. sign in

arxiv: 2510.02857 · v2 · pith:7KIPD7VGnew · submitted 2025-10-03 · ✦ hep-ex

Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb⁻¹ of data collected at sqrt{s}=13 and 13.6 TeV with the ATLAS detector

ATLAS Collaboration This is my paper

Pith reviewed 2026-05-25 07:32 UTC · model grok-4.3

classification ✦ hep-ex
keywords resonance searchscalar particlesHiggs bosondiphoton decaybottom quark decayATLAS experimentLHCnew physics
0
0 comments X

The pith

No significant excess is observed in the search for a heavy scalar X decaying to a lighter scalar S and the Higgs boson.

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

This paper reports a search for the resonant production of a heavy scalar particle X that decays into a lighter scalar S and the Standard Model Higgs boson. The search focuses on the final state where S decays to a pair of bottom quarks and the Higgs decays to two photons, using ATLAS detector data from proton-proton collisions at 13 and 13.6 TeV with a total luminosity of 199 fb^{-1}. The analysis covers a wide range of masses for both X and S, and finds no evidence beyond the expected background. Upper limits are placed on the product of the production cross section and the branching fraction for this process.

Core claim

No significant excess over the Standard Model background prediction is observed in the X → S(→ b b̄) H(→ γγ) channel, allowing 95% confidence level limits on the cross section times branching fraction ranging from 9 fb to 0.06 fb for the process at 13 TeV.

What carries the argument

The two-photon and two-bottom-quark final state selection and mass reconstruction to search for resonances in the X and S mass planes.

If this is right

  • Models predicting additional scalar particles in this mass range are constrained by the upper limits.
  • The search can be extended with more data to probe smaller cross sections.
  • The limits apply specifically to the 13 TeV dataset but similar sensitivities are expected at 13.6 TeV.

Where Pith is reading between the lines

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

  • This result can be combined with searches in other decay channels to further constrain extended Higgs sectors.
  • Future high-luminosity LHC runs could either discover such a resonance or push the limits much lower.
  • If the background modeling assumption holds, these limits provide a benchmark for theoretical models with multiple scalars.

Load-bearing premise

The Standard Model background prediction accurately describes the observed data across the full mass range in the signal regions.

What would settle it

A statistically significant excess in the reconstructed invariant mass distributions of the two photons and two b-jets above the predicted background would falsify the no-signal claim.

read the original abstract

A search for the resonant production of a heavy scalar $X$ decaying into a lighter scalar $S$ and a Higgs boson, through the process $X \rightarrow S (\rightarrow b \bar{b})H ( \rightarrow \gamma\gamma)$, where the two photons are consistent with the Higgs boson decay, is performed. The search is conducted using integrated luminosities of 140 and 59 fb$^{-1}$ of proton-proton collision data at centre-of-mass energies of 13 and 13.6 TeV, respectively, recorded with the ATLAS detector at the LHC. The search is performed over the mass ranges of 170 $\leq$ $m_{X}$ $\leq$ 1000 GeV and 15 $\leq$ $m_{S}$ $\leq$ 500 GeV. No significant excess over the Standard Model background prediction is observed and limits at 95% confidence level are set on the product of cross section and branching fraction for the process $X \rightarrow S (\rightarrow b \bar{b})H ( \rightarrow \gamma\gamma)$ at 13 TeV, ranging from 9 fb to 0.06 fb.

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

0 major / 1 minor

Summary. The manuscript reports a search for resonant production of a heavy scalar X decaying to a lighter scalar S and the Higgs boson via X → S(→bb)H(→γγ) using 140 fb^{-1} at 13 TeV and 59 fb^{-1} at 13.6 TeV recorded with the ATLAS detector. The search covers 170 ≤ m_X ≤ 1000 GeV and 15 ≤ m_S ≤ 500 GeV. No significant excess over the SM background is observed, and 95% CL limits are placed on σ × BR ranging from 9 fb to 0.06 fb.

Significance. This is a standard null-result search in a well-established final state that constrains BSM scenarios with additional scalars. The analysis employs established ATLAS methods including data-driven background estimation for the diphoton + di-b-jet channel. The stress-test concern on background modeling accuracy does not land as a load-bearing issue; the provided description indicates use of simulation plus data-driven techniques with systematic uncertainties, consistent with prior ATLAS publications in this channel.

minor comments (1)
  1. Abstract: the quoted limits are stated to be 'at 13 TeV' while the dataset includes 13.6 TeV data; clarify whether the limits are derived from the 13 TeV sample alone, the combined dataset, or if 13.6 TeV results are presented separately.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of the manuscript and their recommendation to accept. There are no major comments requiring a point-by-point response.

Circularity Check

0 steps flagged

No circularity: standard experimental null-result search with direct data-to-background comparison

full rationale

The paper performs a resonance search in the X → S(→bb)H(→γγ) channel using ATLAS data at 13/13.6 TeV. The central result is the observation of no significant excess over the modeled SM background, followed by 95% CL limits on σ×BR. This follows from direct comparison of observed events to predicted background yields (including data-driven and simulation-based estimates with systematics) across mass ranges, without any parameter fitted to the signal region that is then reinterpreted as a prediction. No equations, ansatze, or self-citations reduce the limit-setting procedure to a tautology or to prior author work by construction. The analysis relies on established experimental methods whose validity is independently testable against control regions and external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on accurate modeling of Standard Model backgrounds and detector response; no free parameters or invented entities are introduced in the abstract.

axioms (1)
  • domain assumption Standard Model background processes are correctly modeled in simulation and data-driven estimates without significant mismodeling in the signal region.
    The 'no significant excess' statement depends directly on this background accuracy.

pith-pipeline@v0.9.0 · 5765 in / 1174 out tokens · 44557 ms · 2026-05-25T07:32:35.587932+00:00 · methodology

Review history (2 revisions) →

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Measuring gravitational wave spectrum from electroweak phase transition and Higgs self-couplings

    hep-ph 2025-11 unverdicted novelty 5.0

    Frequency-domain simulations of the Taiji mission, including noise and foregrounds, demonstrate that the stochastic gravitational wave background from an electroweak phase transition can constrain Higgs cubic and quar...

  2. Bayesian analysis of the complex singlet model with phase transition gravitational waves

    hep-ph 2025-11 unverdicted novelty 3.0

    Bayesian forecasts for the Taiji detector constrain complex singlet model parameters through electroweak phase transition gravitational wave signals.

Reference graph

Works this paper leans on

89 extracted references · 89 canonical work pages · cited by 2 Pith papers · 47 internal anchors

  1. [1]

    ATLAS Collaboration,Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, Phys. Lett. B716(2012) 1, arXiv:1207.7214 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  2. [2]

    CMS Collaboration, Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC, Phys. Lett. B716(2012) 30, arXiv:1207.7235 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  3. [3]

    Complex Singlet Extension of the Standard Model

    V. Barger, P. Langacker, M. McCaskey, M. Ramsey-Musolf and G. Shaughnessy, Complex singlet extension of the standard model, Phys. Rev. D79(2009) 015018, arXiv:0811.0393 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2009

  4. [4]

    Robens, T

    T. Robens, T. Stefaniak and J. Wittbrodt, Two-real-scalar-singlet extension of the SM: LHC phenomenology and benchmark scenarios, Eur. Phys. J. C80(2020) 151, arXiv:1908.08554 [hep-ph]

    work page arXiv 2020

  5. [5]

    Papaefstathiou, T

    A. Papaefstathiou, T. Robens and G. Tetlalmatzi-Xolocotzi, Triple Higgs boson production at the Large Hadron Collider with Two Real Singlet scalars, JHEP05(2021) 193, arXiv:2101.00037 [hep-ph]

    work page arXiv 2021

  6. [6]

    I. F. Ginzburg, M. Krawczyk and P. Osland,Two-Higgs-Doublet Models with CP violation, 2002, arXiv:hep-ph/0211371 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2002

  7. [7]

    X.-G. He, T. Li, X.-Q. Li, J. Tandean and H.-C. Tsai, Constraints on scalar dark matter from direct experimental searches, Phys. Rev. D79(2009) 023521, arXiv:0811.0658 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2009

  8. [8]

    Mühlleitner, M

    M. Mühlleitner, M. O. P. Sampaio, R. Santos and J. Wittbrodt, The N2HDM under theoretical and experimental scrutiny, JHEP03(2017) 94, arXiv:1612.01309 [hep-ph]

    work page arXiv 2017

  9. [9]

    The Next-to-Minimal Supersymmetric Standard Model

    U. Ellwanger, C. Hugonie and A. M. Teixeira, The Next-to-Minimal Supersymmetric Standard Model, Phys. Rept.496(2010) 1, arXiv:0910.1785 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2010

  10. [10]

    The Next-to-Minimal Supersymmetric extension of the Standard Model reviewed

    M. Maniatis,The next-to-minimal supersymmetric extension of the standard model reviewed, Int. J. Mod. Phys. A25(2010), arXiv:0906.0777 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2010

  11. [11]

    CMS Collaboration,Search for a massive scalar resonance decaying to a light scalar and a Higgs boson in the four𝑏quarks final state with boosted topology, Phys. Lett. B842(2023) 137392, arXiv:2204.12413 [hep-ex]

    work page arXiv 2023

  12. [12]

    CMS Collaboration,Search for a heavy Higgs boson decaying into two lighter Higgs bosons in the 𝜏𝜏𝑏𝑏final state at13TeV, JHEP11(2021) 057, arXiv:2106.10361 [hep-ex]

    work page arXiv 2021

  13. [13]

    CMS Collaboration,Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton–proton collisions at√𝑠=13TeV, JHEP05(2024) 316, arXiv:2310.01643 [hep-ex]

    work page arXiv 2024

  14. [14]

    Rept.1115(2025) 368, arXiv:2403.16926 [hep-ex]

    CMS Collaboration,Searches for Higgs boson production through decays of heavy resonances, Phys. Rept.1115(2025) 368, arXiv:2403.16926 [hep-ex]. 16

    work page arXiv 2025

  15. [15]

    ATLAS Collaboration, Search for a resonance decaying into a scalar particle and a Higgs boson in final states with leptons and two photons in proton–proton collisions at√𝑠=13TeV with the ATLAS detector, JHEP10(2024) 104, arXiv:2405.20926 [hep-ex]

    work page arXiv 2024

  16. [16]

    ATLAS Collaboration, Search for a new heavy scalar particle decaying into a Higgs boson and a new scalar singlet in final states with one or two light leptons and a pair of𝜏-leptons with the ATLAS detector, JHEP10(2023) 009, arXiv:2307.11120 [hep-ex]

    work page arXiv 2023

  17. [17]

    ATLAS Collaboration,Search for triple Higgs boson production in the6𝑏final state using𝑝 𝑝 collisions at√𝑠=13TeV with the ATLAS detector, Phys. Rev. D111(2025) 032006, arXiv:2411.02040 [hep-ex]

    work page arXiv 2025

  18. [18]

    ATLAS Collaboration, Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons in proton–proton collisions at√𝑠=13TeV with the ATLAS detector, JHEP11(2024) 047, arXiv:2404.12915 [hep-ex]

    work page arXiv 2024

  19. [19]

    CMS Collaboration, Search for a new scalar resonance decaying to a Higgs boson and another new scalar particle in the final state with two bottom quarks and two photons in proton-proton collisions at√𝑠= 13 TeV, (2025), arXiv:2508.11494 [hep-ex]

    work page arXiv 2025

  20. [20]

    ATLAS Collaboration,The ATLAS Experiment at the CERN Large Hadron Collider, JINST3(2008) S08003

    work page 2008

  21. [21]

    ATLAS Collaboration,The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3, JINST19(2024) P05063, arXiv:2305.16623 [physics.ins-det]

    work page arXiv 2024

  22. [22]

    ATLAS Collaboration,Performance of the ATLAS trigger system in 2015, Eur. Phys. J. C77(2017) 317, arXiv:1611.09661 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  23. [23]

    ATLAS Collaboration,The ATLAS trigger system for LHC Run 3 and trigger performance in 2022, JINST19(2024) P06029, arXiv:2401.06630 [hep-ex]

    work page arXiv 2022

  24. [24]

    ATLAS Collaboration,Software and computing for Run 3 of the ATLAS experiment at the LHC, Eur. Phys. J. C85(2025) 234, arXiv:2404.06335 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2025

  25. [25]

    ATLAS Collaboration,ATLAS data quality operations and performance for 2015–2018 data-taking, JINST15(2020) P04003, arXiv:1911.04632 [physics.ins-det]

    work page arXiv 2015

  26. [26]

    ATLAS Collaboration, Luminosity determination in𝑝 𝑝collisions at√𝑠=13TeV using the ATLAS detector at the LHC, Eur. Phys. J. C83(2023) 982, arXiv:2212.09379 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2023

  27. [27]

    ATLAS Collaboration, Preliminary analysis of the luminosity calibration for the ATLAS13.6TeV data recorded in 2023, ATL-DAPR-PUB-2024-001, 2024,url:https://cds.cern.ch/record/2900949

    work page arXiv 2023

  28. [28]

    ATLAS Collaboration,Performance of electron and photon triggers in ATLAS during LHC Run 2, Eur. Phys. J. C80(2020) 47, arXiv:1909.00761 [hep-ex]

    work page arXiv 2020

  29. [29]

    ATLAS Collaboration,Electron and photon performance measurements with the ATLAS detector using the 2015–2017 LHC proton–proton collision data, JINST14(2019) P12006, arXiv:1908.00005 [hep-ex]. 17

    work page arXiv 2015

  30. [30]

    A comprehensive guide to the physics and usage of PYTHIA 8.3

    C. Bierlich et al.,A comprehensive guide to the physics and usage of PYTHIA 8.3, SciPost Phys. Codebases (2022) 8, arXiv:2203.11601 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2022

  31. [31]

    NNPDF Collaboration, R. D. Ball et al.,Parton distributions with LHC data, Nucl. Phys. B867(2013) 244, arXiv:1207.1303 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2013

  32. [32]

    ATLAS Collaboration,ATLAS Pythia 8 tunes to7TeV data, ATL-PHYS-PUB-2014-021, 2014, url:https://cds.cern.ch/record/1966419

    work page arXiv 2014

  33. [33]

    ATLAS Collaboration,Combination of Searches for Resonant Higgs Boson Pair Production Using 𝑝 𝑝Collisions at √𝑠=13TeV with the ATLAS Detector, Phys. Rev. Lett.132(2024) 231801, arXiv:2311.15956 [hep-ex]

    work page arXiv 2024

  34. [34]

    Bothmann et al.,Event generation with Sherpa 2.2, SciPost Phys.7(2019) 034, arXiv:1905.09127 [hep-ph]

    E. Bothmann et al.,Event generation with Sherpa 2.2, SciPost Phys.7(2019) 034, arXiv:1905.09127 [hep-ph]

    work page arXiv 2019

  35. [35]

    Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector

    D. de Florian et al., Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector, (2017), arXiv:1610.07922 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2017

  36. [36]

    HDECAY: a Program for Higgs Boson Decays in the Standard Model and its Supersymmetric Extension

    A. Djouadi, J. Kalinowski and M. Spira,HDECAY: a program for Higgs boson decays in the Standard Model and its supersymmetric extension, Comput. Phys. Commun.108(1998) 56, arXiv:hep-ph/9704448

    work page internal anchor Pith review Pith/arXiv arXiv 1998

  37. [37]

    Parton Ladder Splitting and the Rapidity Dependence of Transverse Momentum Spectra in Deuteron-Gold Collisions at RHIC

    K. Werner, F.-M. Liu and T. Pierog, Parton ladder splitting and the rapidity dependence of transverse momentum spectra in deuteron-gold collisions at the BNL Relativistic Heavy Ion Collider, Phys. Rev. C74(2006) 044902, arXiv:hep-ph/0506232 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2006

  38. [38]

    EPOS LHC : test of collective hadronization with LHC data

    T. Pierog, I. Karpenko, J. M. Katzy, E. Yatsenko and K. Werner,EPOS LHC: Test of collective hadronization with data measured at the CERN Large Hadron Collider, Phys. Rev. C92(2015) 034906, arXiv:1306.0121 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  39. [39]

    ATLAS Collaboration,The Pythia 8 A3 tune description of ATLAS minimum bias and inelastic measurements incorporating the Donnachie–Landshoff diffractive model, ATL-PHYS-PUB-2016-017, 2016,url:https://cds.cern.ch/record/2206965

    work page arXiv 2016

  40. [40]

    D. J. Lange,The EvtGen particle decay simulation package, Nucl. Instrum. Meth. A462(2001) 152

    work page 2001

  41. [41]

    ATLAS Collaboration,The ATLAS Simulation Infrastructure, Eur. Phys. J. C70(2010) 823, arXiv:1005.4568 [physics.ins-det]

    work page internal anchor Pith review Pith/arXiv arXiv 2010

  42. [42]

    Agostinelli et al.,Geant4– a simulation toolkit, Nucl

    S. Agostinelli et al.,Geant4– a simulation toolkit, Nucl. Instrum. Meth. A506(2003) 250

    work page 2003

  43. [43]

    ATLAS Collaboration,AtlFast3: The Next Generation of Fast Simulation in ATLAS, Comput. Softw. Big Sci.6(2022) 7, arXiv:2109.02551 [hep-ex]

    work page arXiv 2022

  44. [44]

    J. Alwall et al.,The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations, JHEP07(2014) 079, arXiv:1405.0301 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2014

  45. [45]

    NNPDF Collaboration, R. D. Ball et al.,Parton distributions for the LHC run II, JHEP04(2015) 040, arXiv:1410.8849 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  46. [46]

    ATLAS Collaboration,Measurement of the𝑍/𝛾 ∗ boson transverse momentum distribution in𝑝 𝑝 collisions at√𝑠=7TeV with the ATLAS detector, JHEP09(2014) 145, arXiv:1406.3660 [hep-ex]. 18

    work page internal anchor Pith review Pith/arXiv arXiv 2014

  47. [47]

    MINLO: Multi-scale improved NLO

    K. Hamilton, P. Nason and G. Zanderighi,MINLO: multi-scale improved NLO, JHEP10(2012) 155, arXiv:1206.3572 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  48. [48]

    J. M. Campbell et al.,NLO Higgs boson production plus one and two jets using the POWHEG BOX, MadGraph4 and MCFM, JHEP07(2012) 092, arXiv:1202.5475 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  49. [49]

    Merging H/W/Z + 0 and 1 jet at NLO with no merging scale: a path to parton shower + NNLO matching

    K. Hamilton, P. Nason, C. Oleari and G. Zanderighi,Merging H/W/Z + 0 and 1 jet at NLO with no merging scale: a path to parton shower + NNLO matching, JHEP05(2013) 082, arXiv:1212.4504 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2013

  50. [50]

    Transverse-momentum resummation and the spectrum of the Higgs boson at the LHC

    G. Bozzi, S. Catani, D. de Florian and M. Grazzini, Transverse-momentum resummation and the spectrum of the Higgs boson at the LHC, Nucl. Phys. B737(2006) 73, arXiv:hep-ph/0508068

    work page internal anchor Pith review Pith/arXiv arXiv 2006

  51. [51]

    Transverse-momentum resummation: Higgs boson production at the Tevatron and the LHC

    D. de Florian, G. Ferrera, M. Grazzini and D. Tommasini, Transverse-momentum resummation: Higgs boson production at the Tevatron and the LHC, JHEP11(2011) 064, arXiv:1109.2109 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2011

  52. [52]

    PDF4LHC recommendations for LHC Run II

    J. Butterworth et al.,PDF4LHC recommendations for LHC Run II, J. Phys. G43(2016) 023001, arXiv:1510.03865 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  53. [53]

    A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms

    P. Nason,A new method for combining NLO QCD with shower Monte Carlo algorithms, JHEP11(2004) 040, arXiv:hep-ph/0409146

    work page internal anchor Pith review Pith/arXiv arXiv 2004

  54. [54]

    Matching NLO QCD computations with Parton Shower simulations: the POWHEG method

    S. Frixione, P. Nason and C. Oleari, Matching NLO QCD computations with parton shower simulations: the POWHEG method, JHEP11(2007) 070, arXiv:0709.2092 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2007

  55. [55]

    A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX

    S. Alioli, P. Nason, C. Oleari and E. Re,A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX, JHEP06(2010) 043, arXiv:1002.2581 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2010

  56. [56]

    NLO Higgs boson production via vector-boson fusion matched with shower in POWHEG

    P. Nason and C. Oleari, NLO Higgs boson production via vector-boson fusion matched with shower in POWHEG, JHEP02(2010) 037, arXiv:0911.5299 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2010

  57. [57]

    Higher Order QCD predictions for Associated Higgs production with anomalous couplings to gauge bosons

    K. Mimasu, V. Sanz and C. Williams,Higher order QCD predictions for associated Higgs production with anomalous couplings to gauge bosons, JHEP08(2016) 039, arXiv:1512.02572 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  58. [58]

    HW/HZ + 0 and 1 jet at NLO with the POWHEG BOX interfaced to GoSam and their merging within MiNLO

    G. Luisoni, P. Nason, C. Oleari and F. Tramontano,𝐻𝑊±/𝐻 𝑍+ 0 and 1 jet at NLO with the POWHEG BOX interfaced to GoSam and their merging within MiNLO, JHEP10(2013) 083, arXiv:1306.2542 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2013

  59. [59]

    H. B. Hartanto, B. Jäger, L. Reina and D. Wackeroth, Higgs boson production in association with top quarks in the POWHEG BOX, Phys. Rev. D91(2015) 094003, arXiv:1501.04498 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  60. [60]

    NLO predictions for Higgs boson pair production with full top quark mass dependence matched to parton showers

    G. Heinrich, S. P. Jones, M. Kerner, G. Luisoni and E. Vryonidou,NLO predictions for Higgs boson pair production with full top quark mass dependence matched to parton showers, JHEP08(2017) 088, arXiv:1703.09252 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2017

  61. [61]

    Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects

    G. Heinrich, S. Jones, M. Kerner, G. Luisoni and L. Scyboz,Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects, JHEP06(2019) 066, arXiv:1903.08137 [hep-ph]. 19

    work page internal anchor Pith review Pith/arXiv arXiv 2019

  62. [62]

    ATLAS Collaboration,Electron and photon efficiencies in LHC Run 2 with the ATLAS experiment, JHEP05(2024) 162, arXiv:2308.13362 [hep-ex]

    work page arXiv 2024

  63. [63]

    ATLAS Collaboration, Tools for estimating fake/non-prompt lepton backgrounds with the ATLAS detector at the LHC, JINST18(2023) T11004, arXiv:2211.16178 [hep-ex]

    work page arXiv 2023

  64. [64]

    The anti-k_t jet clustering algorithm

    M. Cacciari, G. P. Salam and G. Soyez,The anti-𝑘𝑡 jet clustering algorithm, JHEP04(2008) 063, arXiv:0802.1189 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2008

  65. [65]

    FastJet user manual

    M. Cacciari, G. P. Salam and G. Soyez,FastJet user manual, Eur. Phys. J. C72(2012) 1896, arXiv:1111.6097 [hep-ph]

    work page internal anchor Pith review Pith/arXiv arXiv 2012

  66. [66]

    ATLAS Collaboration, Jet reconstruction and performance using particle flow with the ATLAS Detector, Eur. Phys. J. C77(2017) 466, arXiv:1703.10485 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2017

  67. [67]

    ATLAS Collaboration, Topological cell clustering in the ATLAS calorimeters and its performance in LHC Run 1, Eur. Phys. J. C77(2017) 490, arXiv:1603.02934 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2017

  68. [68]

    ATLAS Collaboration,Jet energy scale and resolution measured in proton–proton collisions at√𝑠=13TeV with the ATLAS detector, Eur. Phys. J. C81(2021) 689, arXiv:2007.02645 [hep-ex]

    work page arXiv 2021

  69. [69]

    ATLAS Collaboration,Performance of pile-up mitigation techniques for jets in𝑝 𝑝collisions at√𝑠=8TeV using the ATLAS detector, Eur. Phys. J. C76(2016) 581, arXiv:1510.03823 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  70. [70]

    ATLAS Collaboration,Forward jet vertex tagging using the particle flow algorithm, ATL-PHYS-PUB-2019-026, 2019,url:https://cds.cern.ch/record/2683100

    work page arXiv 2019

  71. [71]

    ATLAS Collaboration,Transforming jet flavour tagging at ATLAS, (2025), arXiv:2505.19689 [hep-ex]

    work page arXiv 2025

  72. [72]

    ATLAS Collaboration,ATLAS flavour-tagging algorithms for the LHC Run 2𝑝 𝑝collision dataset, Eur. Phys. J. C83(2023) 681, arXiv:2211.16345 [physics.data-an]

    work page arXiv 2023

  73. [73]

    ATLAS Collaboration,Study of Higgs boson pair production in the𝐻𝐻→𝑏¯𝑏𝛾𝛾final state with 308fb −1 of data collected at√𝑠=13TeV and13.6TeV by the ATLAS experiment, (2025), arXiv:2507.03495 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2025

  74. [74]

    ATLAS Collaboration,Muon reconstruction and identification efficiency in ATLAS using the full Run 2𝑝 𝑝collision data set at√𝑠=13TeV, Eur. Phys. J. C81(2021) 578, arXiv:2012.00578 [hep-ex]

    work page arXiv 2021

  75. [75]

    Parameterized Machine Learning for High-Energy Physics

    P. Baldi, K. Cranmer, T. Faucett, P. Sadowski and D. Whiteson, Parameterized neural networks for high-energy physics, Eur. Phys. J. C76(2016) 235, arXiv:1601.07913 [hep-ex]

    work page internal anchor Pith review Pith/arXiv arXiv 2016

  76. [76]

    Chollet et al.,Keras, 2015,url:https://keras.io

    F. Chollet et al.,Keras, 2015,url:https://keras.io

    work page 2015

  77. [77]

    Garnett,Bayesian Optimization, Cambridge University Press, 2023,isbn: 978-1-108-42578-0

    R. Garnett,Bayesian Optimization, Cambridge University Press, 2023,isbn: 978-1-108-42578-0

    work page 2023

  78. [78]

    ATLAS Collaboration,Search for Higgs boson pair production in the two bottom quarks plus two photons final state in𝑝 𝑝collisions at√𝑠=13TeV with the ATLAS detector, Phys. Rev. D106(2022) 052001, arXiv:2112.11876 [hep-ex]. 20

    work page arXiv 2022

  79. [79]

    ATLAS Collaboration,Studies of new Higgs boson interactions through nonresonant𝐻𝐻 production in the𝑏¯𝑏𝛾𝛾final state in𝑝 𝑝collisions at √𝑠=13TeV with the ATLAS detector, JHEP01(2024) 066, arXiv:2310.12301 [hep-ex]

    work page arXiv 2024

  80. [80]

    A. D. Bukin,Fitting function for asymmetric peaks, (2007), arXiv:0711.4449 [physics.data-an]

    work page internal anchor Pith review Pith/arXiv arXiv 2007

Showing first 80 references.