Abstract

With the increase in energy of the Large Hadron Collider to a centre-of-mass energy of 13 text {TeV} for Run 2, events with dense environments, such as in the cores of high-energy jets, became a focus for new physics searches as well as measurements of the Standard Model. These environments are characterized by charged-particle separations of the order of the tracking detectors sensor granularity. Basic track quantities are compared between 3.2 fb^{-1} of data collected by the ATLAS experiment and simulation of proton–proton collisions producing high-transverse-momentum jets at a centre-of-mass energy of 13 text {TeV}. The impact of charged-particle separations and multiplicities on the track reconstruction performance is discussed. The track reconstruction efficiency in the cores of jets with transverse momenta between 200 and 1600 text {GeV} is quantified using a novel, data-driven, method. The method uses the energy loss, {text { d}}{} textit{E}/dtextit{x}, to identify pixel clusters originating from two charged particles. Of the charged particles creating these clusters, the measured fraction that fail to be reconstructed is 0.061 pm 0.006 {text {(stat.)}} pm 0.014 {text {(syst.)}} and 0.093 pm 0.017 {text {(stat.)}}pm 0.021 {text {(syst.)}} for jet transverse momenta of 200–400 text {GeV} and 1400–1600 text {GeV}, respectively.

Highlights

  • This paper first describes the ATLAS detector (Sect. 2)

  • Extending these mainly Monte Carlo (MC) simulation-based studies, a fully data-driven method is introduced in Sect. 6 which probes the fraction of tracks lost in reconstruction, due to the high density and collimation of charged particles in high-transverse-momentum1 jets

  • This is due to the coarser segmentation of the silicon microstrip detector (SCT) strips in one dimension and the lack of charge information hindering the identification of merged SCT clusters

Read more

Summary

Introduction

This paper first describes the ATLAS detector (Sect. 2). a general overview of the track reconstruction algorithm (Sect. 3) is given, focusing on the performance of charged-particle reconstruction in dense environments at the start of Run 2. The data set utilized is described in Sect. 5), and comparisons between simulation and data are performed in events with energetic jets. Extending these mainly Monte Carlo (MC) simulation-based studies, a fully data-driven method is introduced in Sect. 6 which probes the fraction of tracks lost in reconstruction, due to the high density and collimation of charged particles in high-transverse-momentum ( pT) jets. This is achieved by using the ionization energy loss (dE/dx) in the pixel detector

The ATLAS detector
ATLAS track reconstruction
Clusterization
Iterative combinatorial track finding
Track candidates and ambiguity solving
Neural–network pixel clustering
Track fit
Data and Monte Carlo samples
Track reconstruction performance in dense environments
Classification
Data and MC simulation comparison
Performance for collimated tracks
Performance for tracks in jets
Measurement of track reconstruction efficiency in jets from data
Track selection
Fit method
Systematic uncertainties
Results
Conclusion
Methods
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call