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Factorization for Jet Radius Logarithms in Jet Mass Spectra at the LHC

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arxiv 1605.08038 v2 pith:BORMHN2H submitted 2016-05-25 hep-ph

classification hep-ph
keywords masslogarithmsspectrumlargeradiusdiscussfactorizationresummation
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

To predict the jet mass spectrum at a hadron collider it is crucial to account for the resummation of logarithms between the transverse momentum of the jet and its invariant mass $m_J$. For small jet areas there are additional large logarithms of the jet radius $R$, which affect the convergence of the perturbative series. We present an analytic framework for exclusive jet production at the LHC which gives a complete description of the jet mass spectrum including realistic jet algorithms and jet vetoes. It factorizes the scales associated with $m_J$, $R$, and the jet veto, enabling in addition the systematic resummation of jet radius logarithms in the jet mass spectrum beyond leading logarithmic order. We discuss the factorization formulae for the peak and tail region of the jet mass spectrum and for small and large $R$, and the relations between the different regimes and how to combine them. Regions of experimental interest are classified which do not involve large nonglobal logarithms. We also present universal results for nonperturbative effects and discuss various jet vetoes.

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Cited by 2 Pith papers

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

  1. Extracting Essential Non-perturbative Information in Jet Invariant Mass via the Bayesian Analysis

    hep-ph 2025-07 conditional novelty 7.0 of 10

    A new 3D non-perturbative jet-mass model, fitted to pp data, separates hadronization, ISR, and underlying-event effects and correctly predicts e+e- jet mass data.

  2. One-Point energy correlator inside jets

    hep-ph 2025-07 conditional novelty 4.0 of 10

    A TMD factorization and NNLL resummation is derived for a one-point energy correlator inside jets, and the normalized observable mainly depends on the jet scale, with sensitivity to gluon TMDFFs.

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