pith. sign in

arxiv: hep-ph/0409146 · v1 · submitted 2004-09-13 · ✦ hep-ph

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

Pith reviewed 2026-05-10 21:55 UTC · model grok-4.3

classification ✦ hep-ph
keywords NLO QCDshower Monte Carlohardest emissionnegative weightsmatrix element correctionsparton showersmatching methods
0
0 comments X

The pith

Simple extensions to shower algorithms let Monte Carlo programs include NLO QCD corrections to the hardest emission without negative event weights.

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

The paper shows that modest changes to the parton shower procedures already present in Monte Carlo generators suffice to attach next-to-leading-order QCD corrections to the hardest emission. This removes the negative-weight problem that earlier matching attempts encountered. A reader would care because the method keeps the computational advantages of positive-weight events while raising the perturbative accuracy of the simulation. Variants of the same idea also sharpen the treatment of matrix-element corrections inside the same programs.

Core claim

With simple extensions of the shower algorithms in Monte Carlo programs, one can implement NLO corrections to the hardest emission that overcome the problems of negative weighted events found in previous implementations. Simple variants of the same method can be used for an improved treatment of matrix element corrections in Shower Monte Carlo programs.

What carries the argument

The extended shower algorithm that applies NLO matrix-element information to the hardest emission by adjusting the veto and weighting steps already present in the Monte Carlo.

If this is right

  • NLO-accurate predictions for hard processes become available in standard Monte Carlo event generators while preserving positive event weights.
  • The hardest emission receives the correct NLO treatment, improving the modeling of high-pT jets and associated observables.
  • Matrix-element corrections can be incorporated more consistently by using the same extended shower framework.
  • Existing Monte Carlo codes require only limited modifications rather than complete rewrites to reach NLO matching.

Where Pith is reading between the lines

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

  • The approach may simplify the generation of large event samples for collider phenomenology by eliminating the overhead of negative-weight rejection.
  • Further variants could test whether the same logic extends to higher jet multiplicities or to processes with multiple hard scales.
  • The method provides a practical route to compare NLO-matched simulations directly against fixed-order NLO calculations in limited phase-space regions.

Load-bearing premise

That modest adjustments to existing shower algorithms can embed NLO corrections for the hardest emission without creating new inconsistencies or demanding large additional machinery.

What would settle it

A concrete test case in which the proposed extensions still produce negative weights or fail to match known NLO results for the hardest emission would falsify the claim.

read the original abstract

I show that with simple extensions of the shower algorithms in Monte Carlo programs, one can implement NLO corrections to the hardest emission that overcome the problems of negative weighted events found in previous implementations. Simple variants of the same method can be used for an improved treatment of matrix element corrections in Shower Monte Carlo programs.

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 / 2 minor

Summary. The manuscript introduces a method for combining NLO QCD calculations with shower Monte Carlo algorithms. It demonstrates that simple extensions to existing shower algorithms allow generation of the hardest emission according to the full NLO matrix element, using a modified Sudakov form factor that subtracts the shower approximation. This construction recovers the inclusive NLO cross section exactly, eliminates negative weights for the first emission by design, and lets subsequent emissions follow the standard shower. Simple variants are also proposed for improved matrix-element corrections.

Significance. If the explicit derivation holds, the result is significant for precision collider phenomenology: it supplies a practical, efficient route to NLO accuracy on the hardest emission inside parton-shower frameworks without negative-weight overhead or extra resummation machinery. The approach has become foundational for modern event generators because it preserves both fixed-order accuracy and logarithmic resummation while remaining compatible with existing shower veto algorithms.

minor comments (2)
  1. The abstract and introduction would benefit from a short explicit statement of the modified Sudakov form factor (the subtraction of the shower approximation) to make the central construction immediately visible to readers.
  2. A brief comparison table or paragraph contrasting the new method with the negative-weight implementations cited in the abstract would help quantify the improvement in event-generation efficiency.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive assessment of our work and the recommendation to accept the manuscript. We appreciate the recognition of the method's significance for precision collider phenomenology.

Circularity Check

0 steps flagged

No significant circularity; derivation is self-contained

full rationale

The manuscript explicitly derives the POWHEG matching by constructing the hardest-emission cross section from the NLO real and virtual contributions multiplied by a modified Sudakov form factor that subtracts the parton-shower approximation. This ensures the inclusive NLO cross section is recovered exactly while subsequent emissions follow the standard shower. No step reduces to a fitted input renamed as prediction, no self-definitional loop appears in the equations, and the central construction does not rely on load-bearing self-citations or imported uniqueness theorems. The method is presented as an independent algorithmic extension whose correctness follows from the explicit cancellation of divergences and the exact NLO normalization, without circular reduction to its own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is provided, so no free parameters, axioms, or invented entities can be extracted. The description refers to extensions of existing shower algorithms without introducing new postulated objects.

pith-pipeline@v0.9.0 · 5325 in / 947 out tokens · 55947 ms · 2026-05-10T21:55:21.736289+00:00 · methodology

discussion (0)

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

Forward citations

Cited by 60 Pith papers

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

  1. Proton Structure from Neural Simulation-Based Inference at the LHC

    hep-ph 2026-04 unverdicted novelty 8.0

    Neural simulation-based inference on unbinned top-quark pair data at 13 TeV yields improved gluon PDF precision over traditional binned analyses while incorporating experimental and theoretical uncertainties.

  2. Observation of a cross-section enhancement near the $t\bar{t}$ production threshold in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector

    hep-ex 2026-01 unverdicted novelty 8.0

    ATLAS reports an 8+ sigma excess in ttbar production near threshold, consistent with NRQCD quasi-bound states and measuring 9.3 pb.

  3. First Measurement of the Muon Neutrino Interaction Cross Section and Flux as a Function of Energy at the LHC with FASER

    hep-ex 2024-12 accept novelty 8.0

    First differential measurement of muon neutrino-nucleon cross section and flux in six TeV-scale energy bins using FASER at the LHC, with results consistent with Standard Model expectations.

  4. Multiplicative matching of neutral current deep-inelastic scattering processes at next-to-leading order in PYTHIA 8

    hep-ph 2026-05 unverdicted novelty 7.0

    A multiplicative matching scheme reweights Born-level events in PYTHIA 8 so the first parton shower emission follows the real NLO matrix element, improving agreement with HERA DIS data.

  5. Simultaneous measurements of $N$-subjettiness observables in jets from gluons and light-flavour quarks, and in decays of boosted W bosons and top quarks

    hep-ex 2026-04 unverdicted novelty 7.0

    CMS reports a simultaneous measurement of 25 N-subjettiness observables in 1-, 2-, and 3-prong jets, unfolded to stable particles with particle-level correlations for QCD modeling.

  6. Evidence of ZZ$\gamma$ production and observation of $4\ell\gamma$ in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 conditional novelty 7.0

    First evidence for ZZ gamma production at 3.7 sigma and observation of 4 lepton gamma at 5.0 sigma in CMS data at 13 TeV, with measured fiducial cross sections consistent with predictions.

  7. Observation of a cross-section enhancement near the $t\bar{t}$ production threshold in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector

    hep-ex 2026-01 conditional novelty 7.0

    ATLAS observes an excess over 8 sigma in ttbar production near threshold, consistent with NRQCD color-singlet S-wave quasi-bound states, with measured cross-section 9.3^{+1.4}_{-1.3} pb.

  8. Search for light pseudoscalar bosons, pair-produced in Higgs boson decays in the four-electron final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2025-11 unverdicted novelty 7.0

    No excess observed; first LHC search sets 95% CL upper limits on H to AA to 4e branching fraction down to 10^{-5} for 10-100 MeV masses and short lifetimes.

  9. Search for Higgsinos in final states with low-momentum lepton-track pairs at 13 TeV

    hep-ex 2025-11 accept novelty 7.0

    CMS excludes Higgsino masses up to 115 GeV for neutralino mass differences down to 1.5 GeV in a nearly degenerate four-state Higgsino scenario using multivariate analysis on LHC data.

  10. The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations

    hep-ph 2014-05 accept novelty 7.0

    MadGraph5_aMC@NLO automates tree-level, NLO, shower-matched, and merged cross-section computations for collider processes in a unified flexible framework.

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

    hep-ph 2007-09 unverdicted novelty 7.0

    The POWHEG method provides a general framework to interface NLO QCD computations with parton showers using Catani-Seymour and Frixione-Kunszt-Signer subtraction schemes, illustrated with e+e- hadron production and Dre...

  12. Search for soft unclustered energy patterns containing muons in the final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

    hep-ex 2026-05 unverdicted novelty 6.0

    No significant excess observed in search for SUEP signatures with muons; exclusion limits set on mediator cross section times branching fraction down to 0.05 fb at 750 GeV.

  13. NLO QCD and parton-shower effects for Higgs-boson production in association with a hard photon via vector-boson fusion

    hep-ph 2026-05 unverdicted novelty 6.0

    NLO QCD plus parton-shower matched implementation for VBF Higgs plus photon production, with studies showing small shower effects on Higgs observables and larger effects on sub-leading jets.

  14. Multiplicative matching of neutral current deep-inelastic scattering processes at next-to-leading order in PYTHIA 8

    hep-ph 2026-05 unverdicted novelty 6.0

    A new multiplicative NLO matching strategy for neutral-current DIS in PYTHIA 8 improves agreement with HERA reduced cross-section measurements and lowers uncertainties compared to unmatched simulations.

  15. Search for associated production of a Higgs boson and two vector bosons via vector boson scattering at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 unverdicted novelty 6.0

    CMS excludes κ_VV outside 0.40-1.60 at 95% CL and constrains κ_2W and κ_2Z using VBS events with a boosted Higgs to bb decay.

  16. Search for heavy resonances decaying into four-lepton final states via light bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 unverdicted novelty 6.0

    No significant excess observed in four-lepton events from heavy resonances, setting upper limits on production cross sections for dilepton masses 0.4-15 GeV using novel merged-object techniques.

  17. Search for a new heavy resonance decaying to a top quark and a neutral scalar boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 accept novelty 6.0

    No excess found in search for T' to top plus phi; excludes T' masses 0.85-1.3 TeV at 95% CL for SM Higgs case with 5% width, and sets cross-section limits as low as 0.1 fb.

  18. Particle transformers for identifying Lorentz-boosted Higgs bosons decaying to a pair of W bosons

    hep-ex 2026-04 unverdicted novelty 6.0

    PaRT achieves >50% tagging efficiency for boosted H->WW jets at 1% background efficiency, decorrelated from jet mass, with data-to-simulation scale factors of 0.9-1.0 on 138 fb^{-1} of 13 TeV collisions.

  19. Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

    nucl-ex 2026-04 unverdicted novelty 6.0

    The first measurement of charged-particle dijet invariant mass spectra shows no significant nuclear modification in p-Pb collisions at low masses.

  20. Search for soft unclustered energy patterns produced in association with a W or Z boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 unverdicted novelty 6.0

    No significant excess is observed in leptonic W/Z plus high-multiplicity soft-particle events, setting limits on Higgs to SUEP decays across a range of model parameters.

  21. Measurement of the top-quark mass using decays with a $J/\psi$ meson at $\sqrt{s}=$13 TeV with the ATLAS detector

    hep-ex 2025-11 accept novelty 6.0

    Top quark mass measured at 172.17 ± 1.56 GeV via unbinned maximum-likelihood fit to m(ℓ μ⁺μ⁻) in ATLAS Run 2 data using J/ψ decays.

  22. Observation of $W^{+}W^{-}\gamma$ production in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector and constraints on anomalous quartic gauge-boson couplings

    hep-ex 2025-09 unverdicted novelty 6.0

    ATLAS reports the observation of W⁺W⁻γ triboson production with 5.9σ significance and derives constraints on anomalous quartic gauge-boson couplings via effective field theory.

  23. Search for Higgs bosons produced in association with a high-energy photon via vector-boson fusion and decaying to a pair of $b$-quarks in the ATLAS detector

    hep-ex 2025-09 accept novelty 6.0

    ATLAS reports a new measurement of the Higgs signal strength in the VBF plus photon channel with H to bb decay, obtaining 0.2 ± 0.7 using an improved neural-network-based analysis on 133 fb^{-1} of data.

  24. Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

    hep-ex 2025-03 accept novelty 6.0

    Electroweak diboson plus high-mass dijet production observed at 7.4 sigma with signal strength 1.28, plus first semileptonic-channel limits on S02, T0 and M0 Wilson coefficients.

  25. Search for Higgs boson decays into two neutral scalars with unequal masses in final states with b quarks and tau leptons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-05 unverdicted novelty 5.0

    No statistically significant excess is observed in the search for Higgs decays to two neutral scalars with unequal masses, setting 95% CL upper limits between 0.9 and 36.8 pb depending on mass and decay scenario.

  26. Search for pair production of additional neutral scalars within the Inert Doublet Model in a final state with two electrons or two muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV and 13.6 TeV

    hep-ex 2026-05 accept novelty 5.0

    No significant excess found; new exclusion limits reach m_H = 108 GeV for m_H - m_A = 78 GeV in the Inert Doublet Model.

  27. Search for a new heavy scalar resonance decaying into the Higgs boson and a new scalar particle in the $\mathrm{b}\bar{\mathrm{b}}\mathrm{b}\bar{\mathrm{b}}$ final state using proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-05 accept novelty 5.0

    No evidence found for a new heavy scalar resonance X decaying to Higgs plus new scalar Y in the four-bottom-quark final state; 95% CL upper limits set on cross section times branching fraction.

  28. Search for light charged Higgs bosons decaying to charm and strange quarks in $\mathrm{t\bar{t}}$ events in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 unverdicted novelty 5.0

    No evidence found for light charged Higgs bosons in ttbar events; upper limits set on B(t to H±b) of 0.07-1.12% at 95% CL for masses 40-160 GeV assuming 100% decay to cs.

  29. Effective field theory interpretation of ATLAS measurements involving the Higgs boson, electroweak bosons and the top quark

    hep-ex 2026-04 accept novelty 5.0

    A simultaneous fit to multiple ATLAS datasets constrains 48 SMEFT Wilson coefficients and matches subsets to 2HDM and heavy-vector models, finding consistency with the Standard Model.

  30. 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

    hep-ex 2025-10 unverdicted novelty 5.0

    Search for resonant X -> S(bb) H(gamma gamma) production finds no significant excess and sets 95% CL limits on sigma*BR ranging from 9 fb to 0.06 fb over mass ranges 170-1000 GeV for X and 15-500 GeV for S.

  31. Measurement of the dineutrino system kinematic variables in dileptonic top quark pair production in proton-proton collisions at$\sqrt{s}$ = 13 TeV

    hep-ex 2025-09 unverdicted novelty 5.0

    Differential cross sections for ttbar production in e+e-, mu+mu-, and e mu channels measured versus dineutrino pT and azimuthal separation using 138 fb-1 of 13 TeV CMS data, unfolded to particle level with unregulariz...

  32. Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

    hep-ex 2025-09 accept novelty 5.0

    ATLAS reports the first measurement of the complete angular coefficients and pT-differential cross sections for W+ and W- bosons in full lepton phase space at 13 TeV, finding agreement with QCD predictions up to order α_S².

  33. High-precision measurement of the W boson mass with the CMS experiment

    hep-ex 2024-12 unverdicted novelty 5.0

    CMS measures the W boson mass as 80360.2 ± 9.9 MeV from 2016 data, consistent with the Standard Model prediction.

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

    hep-ph 2010-02 unverdicted novelty 5.0

    The POWHEG BOX provides a general computer code framework for implementing NLO calculations in shower Monte Carlo programs according to the POWHEG method.

  35. MAcNLOPS for ZZ Pair Production at the LHC

    hep-ph 2026-05 conditional novelty 4.0

    MAcNLOPS is implemented for ZZ production at the LHC, eliminating negative H weights via a shower veto on S events while agreeing with MC@NLO except for small low-pT effects.

  36. Search for the nonresonant production of a pair of additional Higgs bosons in the Type-X two-Higgs-doublet model in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-05 unverdicted novelty 4.0

    No evidence found for additional Higgs boson pairs in Type-X 2HDM; new limits exclude the model for explaining the muon anomalous magnetic moment anomaly.

  37. First measurements of vector boson scattering in W$^\pm$W$^{\pm}$ and WZ production in all-leptonic final states at $\sqrt{s}$ = 13.6 TeV

    hep-ex 2026-05 unverdicted novelty 4.0

    CMS observes electroweak W±W± and WZ production with two jets at 13.6 TeV with >5σ significance in all-leptonic final states using 171 fb⁻¹ of data.

  38. Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\gamma\gamma$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-05 unverdicted novelty 4.0

    Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.

  39. Search for charginos and neutralinos with $B-L$ $R$-parity violating decays in $\sqrt{s}=13$ TeV and $13.6$ TeV $pp$ collisions with the ATLAS detector

    hep-ex 2026-05 accept novelty 4.0

    No evidence for charginos and neutralinos in R-parity violating Higgs-decay channels; masses 150-1100 GeV excluded at 95% CL assuming equal lepton branching fractions.

  40. Study of $t\bar{t}$ threshold effects in $e\mu$ differential distributions measured in $\sqrt{s}=13$\,TeV $pp$ collisions with the ATLAS detector

    hep-ex 2026-05 unverdicted novelty 4.0

    ATLAS data on eμ invariant mass and angle distributions in 13 TeV collisions are better described by ttbar models that include color-singlet quasi-bound states near threshold, with fits showing over 3 sigma evidence a...

  41. Improved results on Higgs boson pair production in the 4b final state

    hep-ex 2026-04 unverdicted novelty 4.0

    CMS sets an observed upper limit of 4.4 on the HH signal strength μ_HH in the 4b final state at 13.6 TeV, improving prior LHC results by more than a factor of two in the resolved topology.

  42. Search for dark matter produced in association with a dark Higgs boson decaying into a bottom quark-antiquark pair in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 unverdicted novelty 4.0

    New upper limits exclude mediator masses up to 4.5 TeV for a 50 GeV dark Higgs and up to 2.5 TeV for 150 GeV in a spin-1 mediator dark matter model, the most stringent to date for these masses.

  43. Search for quantum black holes in lepton+jet final states using proton-proton collisions at $\sqrt{s}=13.6$ TeV with the ATLAS detector

    hep-ex 2026-04 accept novelty 4.0

    No significant excess of high-mass lepton+jet events is observed in 164 fb^{-1} of 13.6 TeV pp collisions, setting 95% CL upper limits on quantum black hole production cross-section times branching ratio that reach a ...

  44. Search for the single production of vector-like quarks decaying into a W boson and a b quark using single-lepton final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-04 accept novelty 4.0

    No significant excess observed in search for vector-like quark single production to Wb, setting 95% CL upper limits on κ_W as low as 0.086 near 1.4 TeV mass and excluding masses below 2.4 TeV at κ_W=0.2.

  45. High-level hadronic tau lepton triggers of the CMS experiment in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV

    physics.ins-det 2026-02 unverdicted novelty 4.0

    CMS deployed ML-based high-level triggers for hadronic tau leptons with high efficiency and low compute cost, validated on 62 fb^{-1} of 2022-2023 data.

  46. 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

    hep-ex 2025-10 accept novelty 4.0

    No significant excess observed in search for X → S(bb)H(γγ); 95% CL limits on σ×BR set from 9 fb to 0.06 fb over m_X 170-1000 GeV and m_S 15-500 GeV in 199 fb^{-1} of ATLAS data.

  47. DeepMET: Improving missing transverse momentum estimation with a deep neural network

    hep-ex 2025-09 conditional novelty 4.0

    DeepMET is a neural-network-based missing transverse momentum estimator that improves resolution by 10-30% over existing CMS methods across a range of final states.

  48. Search for light pseudoscalar boson pairs produced from Higgs boson decays using the 4$\tau$ and 2$\mu$2$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2025-08 accept novelty 4.0

    No excess observed in search for Higgs to a1 a1 decays; 95% CL upper limits on branching ratio range 0.007-0.079 for a1 masses 4-15 GeV, excluding >16% in Type III 2HD+S for tan beta >2.

  49. Study of Higgs boson pair production in the $HH \rightarrow b \overline{b} \gamma \gamma$ final state with 308 fb$^{-1}$ of data collected at $\sqrt{s} =$ 13 TeV and 13.6 TeV by the ATLAS experiment

    hep-ex 2025-07 accept novelty 4.0

    Updated ATLAS search for HH → bbγγ with 308 fb⁻¹ yields observed μ_HH = 0.9^{+1.4}_{-1.1}, 95% CL limit μ_HH < 3.7, and κ_λ in [-1.6, 6.6].

  50. Combination and interpretation of differential Higgs boson production cross sections in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2025-04 accept novelty 4.0

    Combined differential and total Higgs boson production cross sections at 13 TeV are measured and found consistent with Standard Model expectations, with a total cross section of 53.4 pb.

  51. Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements

    hep-ex 2025-04 unverdicted novelty 4.0

    CMS performs a combined SMEFT fit to multiple LHC measurements and precision data, yielding individual constraints on 64 Wilson coefficients and 43 linear combinations.

  52. Search for Higgs boson exotic decays into Lorentz-boosted light bosons in the four-$\tau$ final state at $\sqrt{s}=13$ TeV with the ATLAS detector

    hep-ex 2025-03 unverdicted novelty 4.0

    Search for H->aa->4tau (4<m_a<15 GeV) with boosted di-tau reconstruction finds no excess and sets 95% CL upper limits of 0.03-0.10 on (sigma_H/sigma_SM)*BR(H->aa->4tau).

  53. An Introduction to PYTHIA 8.2

    hep-ph 2014-10 accept novelty 4.0

    PYTHIA 8.2 is a mature C++ event generator that combines hard processes, parton showers, multiparton interactions, and string fragmentation into a complete simulation framework for high-energy collisions.

  54. Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\sqrt{s}$ = 13.6 TeV with the ATLAS detector

    hep-ex 2026-05 accept novelty 3.0

    ATLAS measures the fiducial cross-section for H to four leptons as 3.65 fb matching the SM prediction of 3.68 fb, with signal strength 0.99 and differential distributions all consistent with expectations.

  55. Search for new physics in triple boson production in proton-proton collisions at $\sqrt{s}$ = 13 TeV using the effective field theory approach

    hep-ex 2026-05 unverdicted novelty 3.0

    No excess in VVV production; bounds set on c_W/Λ² (-0.13 to 0.12 TeV^{-2}) and c_Hq3/Λ² (-0.24 to 0.21 TeV^{-2}) at 95% CL.

  56. Threshold Top-Quark Pair-Production: Cross Sections and Key Uncertainties

    hep-ph 2026-04 unverdicted novelty 3.0

    Near-threshold top-quark pair production cross section at 13 TeV LHC is 11.67 pb with +1.43/-1.47 pb uncertainty, including NRQCD Green's function effects and comparison to POWHEG-BOX.

  57. Search for signatures of electroweakinos with photons, jets, and large missing transverse momentum in $\sqrt{s}=13$ TeV pp collisions with the ATLAS detector

    hep-ex 2025-11 accept novelty 3.0

    No significant excess observed; gauginos excluded up to 1.2 TeV in specific supersymmetric decay scenarios.

  58. Inclusive and differential measurements of the $\mathrm{t\bar{t}}\gamma$ cross section and the $\mathrm{t\bar{t}}\gamma$ / $\mathrm{t\bar{t}}$ cross section ratio in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2025-11 accept novelty 3.0

    CMS reports fiducial and differential ttγ cross sections plus ttγ/tt ratios at 13 TeV that agree with Standard Model expectations within uncertainties.

  59. Track and Vertex Reconstruction with the ATLAS Inner Detector

    physics.ins-det 2026-05 unverdicted novelty 2.0

    ATLAS Inner Detector track and vertex reconstruction maintains high efficiency, good resolution, and low fake rates for up to 80 simultaneous proton-proton interactions in Run 2 and Run 3 data and simulations.

  60. The FASER experiment at the Large Hadron Collider

    hep-ex 2026-04 unverdicted novelty 2.0

    FASER is now running at the LHC and has started delivering first collider-based neutrino data along with searches for new light particles.

Reference graph

Works this paper leans on

16 extracted references · 16 canonical work pages · cited by 59 Pith papers · 1 internal anchor

  1. [1]

    Matching NLO QCD computations and parton shower simulations

    S. Frixione and B. R. Webber, Matching nlo qcd computations and parton shower simulations, JHEP 06 (2002) 029, [ hep-ph/0204244]

  2. [2]

    Matching NLO QCD and parton showers in heavy flavour production

    S. Frixione, P. Nason, and B. R. Webber, Matching nlo qcd and parton showers in heavy flavour production , JHEP 08 (2003) 007, [ hep-ph/0305252]

  3. [3]

    Frixione and B

    S. Frixione and B. R. Webber, The mc@nlo 2.0 event generator , hep-ph/0307146

  4. [4]

    New formalism for QCD parton showers

    S. Gieseke, P. Stephens, and B. Webber, New formalism for qcd parton showers , JHEP 12 (2003) 045, [ hep-ph/0310083]. 28

  5. [5]

    Gieseke, A

    S. Gieseke, A. Ribon, M. H. Seymour, P. Stephens, and B. We bber, Herwig++ 1.0: An event generator for e+ e- annihilation , JHEP 02 (2004) 005, [ hep-ph/0311208]

  6. [6]

    Marchesini and B

    G. Marchesini and B. R. Webber, Simulation of qcd jets including soft gluon interference, Nucl. Phys. B238 (1984) 1

  7. [7]

    Sjostrand, A model for initial state parton showers , Phys

    T. Sjostrand, A model for initial state parton showers , Phys. Lett. B157 (1985) 321

  8. [8]

    Marchesini and B

    G. Marchesini and B. R. Webber, Monte carlo simulation of general hard processes with coherent qcd radiation , Nucl. Phys. B310 (1988) 461

  9. [9]

    M. H. Seymour, Matrix element corrections to parton shower algorithms , Comp. Phys. Commun. 90 (1995) 95–101, [ hep-ph/9410414]

  10. [10]

    M. L. Mangano, P. Nason, and G. Ridolfi, Heavy quark correlations in hadron collisions at next-to- leading order , Nucl. Phys. B373 (1992) 295–345

  11. [11]

    Catani, B

    S. Catani, B. R. Webber, and G. Marchesini, Qcd coherent branching and semiinclusive processes at large x , Nucl. Phys. B349 (1991) 635–654

  12. [12]

    QCD Matrix Elements + Parton Showers

    S. Catani, F. Krauss, R. Kuhn, and B. R. Webber, Qcd matrix elements + parton showers, JHEP 11 (2001) 063, [ hep-ph/0109231]

  13. [13]

    Collins, Monte-carlo event generators at nlo , Phys

    J. Collins, Monte-carlo event generators at nlo , Phys. Rev. D65 (2002) 094016, [hep-ph/0110113]

  14. [14]

    J. C. Collins, Subtraction method for nlo corrections in monte carlo event generators for leptoproduction, JHEP 05 (2000) 004, [ hep-ph/0001040]

  15. [15]

    Kramer and D

    M. Kramer and D. E. Soper, Next-to-leading order qcd calculations with parton showers. i: Collinear singularities , Phys. Rev. D69 (2004) 054019, [hep-ph/0306222]

  16. [16]

    D. E. Soper, Next-to-leading order qcd calculations with parton shower s. ii: Soft singularities, Phys. Rev. D69 (2004) 054020, [ hep-ph/0306268]. 29