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A comprehensive guide to the physics and usage of PYTHIA 8.3

Mixed citation behavior. Most common role is method (61%).

144 Pith papers citing it
43 external citations · Pith
Method 61% of classified citations
abstract

This manual describes the PYTHIA 8.3 event generator, the most recent version of an evolving physics tool used to answer fundamental questions in particle physics. The program is most often used to generate high-energy-physics collision "events", i.e. sets of particles produced in association with the collision of two incoming high-energy particles, but has several uses beyond that. The guiding philosophy is to produce and reproduce properties of experimentally obtained collisions as accurately as possible. The program includes a wide ranges of reactions within and beyond the Standard Model, and extending to heavy ion physics. Emphasis is put on phenomena where strong interactions play a major role. The manual contains both pedagogical and practical components. All included physics models are described in enough detail to allow the user to obtain a cursory overview of used assumptions and approximations, enabling an informed evaluation of the program output. A number of the most central algorithms are described in enough detail that the main results of the program can be reproduced independently, allowing further development of existing models or the addition of new ones. Finally, a chapter dedicated fully to the user is included towards the end, providing pedagogical examples of standard use cases, and a detailed description of a number of external interfaces. The program code, the online manual, and the latest version of this print manual can be found on the PYTHIA web page: https://www.pythia.org/

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  • abstract This manual describes the PYTHIA 8.3 event generator, the most recent version of an evolving physics tool used to answer fundamental questions in particle physics. The program is most often used to generate high-energy-physics collision "events", i.e. sets of particles produced in association with the collision of two incoming high-energy particles, but has several uses beyond that. The guiding philosophy is to produce and reproduce properties of experimentally obtained collisions as accurately as possible. The program includes a wide ranges of reactions within and beyond the Standard Model, a
  • method for the remaining data, the full range (|𝜂jet|<4.9 ) was used. In order to measure the EMD rate of0𝑛0𝑛 𝛾+𝐴→jets collisions, an additional sample was collected using the same jet trigger requirements but with an L1 ZDC trigger requiring at least one neutron on exactly one side. 5 Several Monte Carlo (MC) samples were produced for this analysis using thePythia8 event generator [45, 46] for the three relevant physical processes:𝛾+𝐴→jets , 𝛾+𝐼 𝑃→jets , and𝛾+𝛾→jets . Final-state stable particles, def
  • method defined in terms of the polar angle𝜃 as 𝜂=−ln tan(𝜃/2) and is equal to the rapidity𝑦=(1/2)ln[(𝐸+𝑝 𝑧)/(𝐸−𝑝 𝑧)] in the relativistic limit. Angular distance is measured in units ofΔ𝑅≡ √︁ (Δ𝑦) 2 + (Δ𝜙) 2. 3 QBH MC signal samples were generated using theQBH v3.02generator [7] to compute the production cross-sections and model the hard-scatter process, assuming zero angular momentum. Events were then interfaced toPythia8 [34] to model parton showering and hadronisation. As in previous iterations of se
  • method focus the discussion on experiments measuring gamma- rays and neutrinos. To accurately determine the expected signal, we first compute the full decay spectrum of the DM candidate using Monte Carlo simulations. We implement our EFT operators inFeynRules[14, 104-106] and simulate the underlying partonic events viaMadGraph5 aMC[107, 108], which is subsequently interfaced withPythia8[109] for parton showering, hadronisation and decay of unstable SM particles. This procedure provides the differential
  • method The following subdominant contributions are also considered: t tW, t tZ and triboson (WWW, WWZ, WZZ) production, simulated with MADGRAPH5 aMC@NLOv2.6.5 at NLO in pQCD [50, 54]. All signal and background processes are simulated using similar Monte Carlo (MC) generator configurations, utilising theNNPDF3.1 [66] NNLO parton distribution functions. All gener- ators are interfaced withPYTHIAv8.240 [67] (v8.306 [68]) for the parton shower simulation, hadronisation, and fragmentation processes for the
  • background Frampton and S.L. Glashow,Unstable heavy particles,Phys. Rev. Lett.44(1980) 1481. [11] P. Gondolo, G. Gelmini and S. Sarkar,Cosmic neutrinos from unstable relic particles,Nucl. Phys. B392(1993) 111 [hep-ph/9209236]. [12] T. Kanzaki, M. Kawasaki, K. Kohri and T. Moroi,Cosmological Constraints on Neutrino Injection,Phys. Rev. D76(2007) 105017 [0705.1200]. [13] Y. Ema, R. Jinno and T. Moroi,Cosmic-Ray Neutrinos from the Decay of Long-Lived Particle and the Recent IceCube Result,Phys. Lett. B733(201
  • method 1) production at1000GeV for Run 2, with slightly higher cross sections for Run 3. The decay branching ratios are set toB ( ˜𝜒± 1 →ℎℓ ±)=100% and B ( ˜𝜒0 1 →ℎ𝜈)=100% , with equal branching fractions to each lepton generation. Samples were generated withMadGraph5_aMC@NLO3.5.3 [39] with theNNPDF3.0nlo[40] parton distribution function (PDF). The parton shower, hadronization, and underlying event were modeled usingPythia8.310 [41] with the A14 set of tuned parameters (tune) [42]. The MC setup for the

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representative citing papers

Dissecting Jet-Tagger Through Mechanistic Interpretability

hep-ph · 2026-05-11 · accept · novelty 8.0

A Particle Transformer jet tagger contains a sparse six-head circuit whose source-relay-readout structure recovers most performance and whose residual stream preferentially encodes 2-prong energy correlators.

Event-axis TMD measurements in $e^+e^-$ and SIDIS

hep-ph · 2026-07-02 · unverdicted · novelty 7.0

Completes soft-operator formulation for thrust-axis TMD in e+e- and SIDIS, proposes nonperturbative model with event-shape dependence, resums logs, and validates against Pythia8.3 simulations.

Putting Jet Substructure on Track(s)

hep-ph · 2026-06-30 · unverdicted · novelty 7.0

First complete NLL calculations of projected energy correlators (up to 4-point) on tracks via factorization theorems and RG evolution, extending prior full-jet results.

Centauric 1-Jettiness in DIS and Universal Power Corrections

hep-ph · 2026-06-18 · unverdicted · novelty 7.0

Introduces Centauric 1-jettiness in DIS, derives N3LL resummation matched to NLO, and establishes universal non-perturbative power corrections scaling as 1/R via reduction to rescaled hemisphere soft function.

Probing jet evolution with charged energy correlators in small systems

nucl-ex · 2026-06-16 · unverdicted · novelty 7.0

Charged energy correlators measured in jets at the LHC show like-sign pairs sensitive to parton shower models and unlike-sign pairs sensitive to hadronization, with charge-independent cold nuclear matter effects in p-Pb collisions.

Decaying spin-3/2 dark matter from baryon number violation

hep-ph · 2026-05-07 · unverdicted · novelty 7.0

Non-supersymmetric spin-3/2 dark matter with baryon-violating portals can explain the relic abundance through UV and Boltzmann-suppressed freeze-in, with viable parameter space constrained by indirect detection, direct detection, and LHC monojet searches.

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Showing 50 of 144 citing papers.