Measurement of the Soft-Drop Jet Mass in pp Collisions at √s=13  TeV with the ATLAS Detector

ATLAS Collaboration

Research output: Contribution to journalArticlepeer-review

46 Citations (Scopus)
142 Downloads (Pure)

Abstract

Jet substructure observables have significantly extended the search program for physics beyond the standard model at the Large Hadron Collider. The state-of-the-art tools have been motivated by theoretical calculations, but there has never been a direct comparison between data and calculations of jet substructure observables that are accurate beyond leading-logarithm approximation. Such observables are significant not only for probing the collinear regime of QCD that is largely unexplored at a hadron collider, but also for improving the understanding of jet substructure properties that are used in many studies at the Large Hadron Collider. This Letter documents a measurement of the first jet substructure quantity at a hadron collider to be calculated at next-to-next-to-leading-logarithm accuracy. The normalized, differential cross section is measured as a function of log10ρ2, where ρ is the ratio of the soft-drop mass to the ungroomed jet transverse momentum. This quantity is measured in dijet events from 32.9  fb−1 of √s=13  TeV proton-proton collisions recorded by the ATLAS detector. The data are unfolded to correct for detector effects and compared to precise QCD calculations and leading-logarithm particle-level Monte Carlo simulations.
Original languageEnglish
Article number092001
JournalPhysical Review Letters
Volume121
DOIs
Publication statusPublished - 22 Nov 2017

Bibliographical note

13 pages plus author list (31 pages total), 3 figures, published in PRL. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/STDM-2017-04/

Keywords

  • hep-ex

Fingerprint

Dive into the research topics of 'Measurement of the Soft-Drop Jet Mass in pp Collisions at √s=13  TeV with the ATLAS Detector'. Together they form a unique fingerprint.

Cite this