Abstract

ABSTRACTObservables which distinguish boosted topologies from QCD jets are playing an increasingly important role at the Large Hadron Collider (LHC). These observables are often used in conjunction with jet grooming algorithms, which reduce contamination from both theoretical and experimental sources. In this paper we derive factorization formulae for groomed multi-prong substructure observables, focusing in particular on the groomed D2 observable, which is used to identify boosted hadronic decays of electroweak bosons at the LHC. Our factorization formulae allow systematically improvable calculations of the perturbative D2 distribution and the resummation of logarithmically enhanced terms in all regions of phase space using renormalization group evolution. They include a novel factorization for the production of a soft subjet in the presence of a grooming algorithm, in which clustering effects enter directly into the hard matching. We use these factorization formulae to draw robust conclusions of experimental relevance regarding the universality of the D2 distribution in both e+e− and pp collisions. In particular, we show that the only process dependence is carried by the relative quark vs. gluon jet fraction in the sample, no non-global logarithms from event-wide correlations are present in the distribution, hadronization corrections are controlled by the perturbative mass of the jet, and all global color correlations are completely removed by grooming, making groomed D2 a theoretically clean QCD observable even in the LHC environment. We compute all ingredients to one-loop accuracy, and present numerical results at next-to-leading logarithmic accuracy for e+e− collisions, comparing with parton shower Monte Carlo simulations. Results for pp collisions, as relevant for phenomenology at the LHC, are presented in a companion paper [1].

Highlights

  • The efficient and robust identification of hadronically-decaying boosted electroweak bosons is a problem of fundamental importance at Run 2 and into the future of the Large Hadron Collider (LHC) physics programme

  • We show that the only process dependence is carried by the relative quark vs. gluon jet fraction in the sample, no non-global logarithms from event-wide correlations are present in the distribution, hadronization corrections are controlled by the perturbative mass of the jet, and all global color correlations are completely removed by grooming, making groomed D2 a theoretically clean QCD observable even in the LHC environment

  • In a companion paper [1] we present D2 distributions for mMDT/soft drop groomed jets produced in pp collisions for processes of phenomenological relevance for jet substructure at the LHC

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Summary

Introduction

The efficient and robust identification of hadronically-decaying boosted electroweak bosons is a problem of fundamental importance at Run 2 and into the future of the Large Hadron Collider (LHC) physics programme. Because of the high-luminosity environment of the LHC, the robust measurement of the substructure of jets requires methods for removing contamination from underlying event, pile-up, or other sources that are mostly uncorrelated with the hard scattering Of these so-called jet grooming techniques, the modified mass drop (mMDT) [27, 28] and soft drop [29] groomers are theoretically most well-understood. The quark or gluon flavor of a jet is well-defined at leading power in zcut 1 These properties imply that the full mMDT/soft drop D2 is only very weakly dependent on the jet mass mJ and the jet energy EJ.

Observables
Energy correlation functions and D2
Phase space and behavior of groomed D2
Review of known results
Groomed jet mass factorization formula
Ungroomed D2 factorization formula
Groomed D2 factorization formula
Unresolved substructure: collinear-soft haze
Resolved substructure: collinear limit
Resolved substructure: soft limit
Merging collinear and soft resolved limits
Matching resolved and unresolved limits
Signal jets
Factorized cross section in pp collisions
Consequences of factorization formulae
Universality of the shape of the D2 distribution
Hadronization corrections suppressed by perturbative jet mass
Grooming efficiency for signal jets
Singular results and comparison with EVENT2
Comparison with parton shower Monte Carlo
Monte Carlo results in pp collisions
Signal distributions
Background distributions
Conclusions
Kinematics and notation
Matrix element definitions
Hard function
Findings
Hard splitting function

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