Jet Reconstruction in CMS using Charged Tracks only



Similar documents
Real Time Tracking with ATLAS Silicon Detectors and its Applications to Beauty Hadron Physics

Top rediscovery at ATLAS and CMS

Vertex and track reconstruction with the ALICE Inner Tracking System

CMS Tracking Performance Results from early LHC Running

Jets energy calibration in ATLAS

Track Trigger and Modules For the HLT

Proton tracking for medical imaging and dosimetry

Measurement of Neutralino Mass Differences with CMS in Dilepton Final States at the Benchmark Point LM9

Tracking/Vertexing/BeamSpot/b-tag Results from First Collisions (TRK )

Top-Quark Studies at CMS

Calorimetry in particle physics experiments

Operation and Performance of the CMS Silicon Tracker

arxiv: v1 [physics.ins-det] 4 Feb 2014

ATLAS NOTE ATLAS-CONF July 21, Search for top pair candidate events in ATLAS at s = 7 TeV. The ATLAS Collaboration.

The TOTEM experiment at the LHC: results and perspective

variables to investigate Monte Carlo methods of t t production

Measurement of the Mass of the Top Quark in the l+ Jets Channel Using the Matrix Element Method

Implications of CMS searches for the Constrained MSSM A Bayesian approach

Validation of the MadAnalysis 5 implementation of ATLAS-SUSY-13-05

The Compact Muon Solenoid Experiment. CMS Note. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. D. J. Mangeol, U.

FTK the online Fast Tracker for the ATLAS upgrade

PHYSICS WITH LHC EARLY DATA

Recent SiD Tracking Studies at CU (and Ancient Outer Tracker Studies at SLAC)

ATLAS Test Beam Analysis in Stockholm: An Overview

Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection -

Delphes, a framework for fast simulation of a general purpose LHC detector

Precision Tracking Test Beams at the DESY-II Synchrotron. Simon Spannagel DPG 2014 T88.7 Mainz,

Highlights of Recent CMS Results. Dmytro Kovalskyi (UCSB)

arxiv:hep-ph/ v2 4 Oct 2003

Electron-Muon Ranger (EMR)

Optimisation of the ATLAS track reconstruction software for Run-2. A. Salzburger, CERN

An option for the SHiP Muon Detector: Scintillator bars with WLS fibers and SiPMs readout

PoS(LHCPP2013)033. Rare B meson decays at LHC. Francesco Dettori Nikhef and Vrij Universiteit, Amsterdam fdettori@nikhef.nl.

CMS Level 1 Track Trigger

arxiv: v1 [hep-ph] 31 Aug 2015

Calorimeter Upgrades for the High Luminosity LHC

Large Hadron Collider am CERN

Information about the T9 beam line and experimental facilities

Fermilab FERMILAB-THESIS

Physik des Higgs Bosons. Higgs decays V( ) Re( ) Im( ) Figures and calculations from A. Djouadi, Phys.Rept. 457 (2008) 1-216

How To Teach Physics At The Lhc

Performance of the CMS cathode strip chambers with cosmic rays

Electron-Muon Ranger (EMR)

JET ENERGY CALIBRATION IN ATLAS

IMPROVEMENT OF JET ENERGY RESOLUTION FOR SEGMENTED HCAL USING LAYER WEIGHTING TECHNIQUE

The LHCb Tracking System. Jeroen van Hunen

Detectors in Nuclear and Particle Physics

The CMS All Silicon Tracker

Jet quenching in heavy-ion collisions at LHC with CMS detector. Yetkin Yilmaz

MICE detectors and first results. M. Bonesini Sezione INFN Milano Bicocca

Cross section, Flux, Luminosity, Scattering Rates

A Guide to Detectors Particle Physics Masterclass. M. van Dijk

Search for Dark Matter at the LHC

The accurate calibration of all detectors is crucial for the subsequent data

Research Management Plan (RMP) for the. STAR Heavy Flavor Tracker (HFT)

Study of the B D* ℓ ν with the Partial Reconstruction Technique

arxiv:nucl-ex/ v2 18 Jul 2005

Theory versus Experiment. Prof. Jorgen D Hondt Vrije Universiteit Brussel jodhondt@vub.ac.be

Progress in understanding quarkonium polarization measurements

Secondary vertex reconstruction from tracking data using the ZEUS-framework t 3-jet reconstruction from ZEUS-data at s = 318 GeV

Concepts in Theoretical Physics

1 Experiments (Brahms, PHENIX, and STAR)

Online CMS Web-Based Monitoring. Zongru Wan Kansas State University & Fermilab (On behalf of the CMS Collaboration)

Tracking systems in HEP:

Running in Luminosity. Mike Lamont Verena Kain

The Mainz LXe TPC MC simulations for a Compton scattering experiment

Image Processing Techniques applied to Liquid Argon Time Projection Chamber(LArTPC) Data

R&D pour le LHC Haute Luminosité

FPGA Online Tracking Algorithm for the PANDA Straw Tube Tracker

A.Besson, IPHC-Strasbourg

EUTelescope: tracking software

GLAST Geant4 Simulation

Transcription:

Jet Reconstruction in CMS using Charged Tracks only Andreas Hinzmann for the CMS Collaboration JET2010 12 Aug 2010

Jet Reconstruction in CMS Calorimeter Jets clustered from calorimeter towers independent detectors Track Jets clustered from tracks Jet plus Tracks correct Calorimeter Jets using momentum of tracks Particle Flow Jets clustered from identified particles reconstructed using all detector components make use of full CMS detector Talk by Sevil Salur 2 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Introduction to TrackJets TrackJets measure the charged component of a jet which typically corresponds to ~60% of the actual quark/gluon momentum Charged jet component is the one measured with the best precision in the tracker TrackJets are a very reliable way to find jets of any energy, down to very low p T (very low fake rate) Jet direction is accurately measured with TrackJets TrackJets are transparent to pile-up, thanks to clean vertex association This talk: Performance of TrackJets, Commissioning using 7 TeV data, First data analyses using TrackJets Documented in CMS PAS JME-10-006 3 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

The CMS detector 4 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

The CMS tracking system Covers η < 2.4 (η = ln[tan(θ/2)]) Pixel detector: 3 barrel layers, 2 forward disks Strip detector: 10-12 barrel and forward layers, ~40% with stereo views Iterative tracking using combinatorial track finder CMS PAS TRK-10-005 5 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

TrackJet reconstruction Select tracks with good momentum error p T > 300 MeV distance to primary vertex (d xy <2mm, d z <5mm) tight cuts on χ 2 /ndof and impact parameter significance TrackJets built by clustering selected tracks using anti-k T algorithm with R = 0.5 separately for each primary vertex 6 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Energy response MC s=14 TeV CMS PAS JME-08-001 Average fraction of charged particles in jets: ~60% 7 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Position resolution CMS PAS JME-10-003 Position resolutions of ~0.04 at p T =10 GeV generator level jets 8 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Reconstruction efficiency Reconstruction efficiency and fake rate studied on MC More than 99% of true GenJets with p T > 15 GeV/c are reconstructed as TrackJets Less than 1% for TrackJets with p T > 10 GeV/c do not correspond to a true GenJet 9 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

TrackJet commissioning March 30, 2010 CMS started collecting data from LHC protonproton collisions at 7 TeV Present results based on 4212310 minimum bias events, corresponding to 100 μb 1 of integrated luminosity Minimum bias events triggered by requiring activity in the beam scintillation detectors on each side of the CMS detector and the reconstruction of one good primary vertex Data is compared to a reference minimum-bias sample produced with the PYTHIA 8.1 event generator and processed with a simulation of the CMS detector response based on GEANT 4. 10 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Inclusive TrackJets p T > 10 GeV Green error-band corresponds to 10% uncertainty on the luminosity Default tune of PYTHIA 8.1 reproduces multiplicity and transverse momentum distribution 11 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Inclusive TrackJets p T > 10 GeV p T > 10 GeV MC and detector simulation reproduces angular distribution of inclusive TrackJets 12 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

TrackJet constituents p T > 10 GeV p T > 10 GeV Median number of tracks per TrackJet: ~6 Median fraction of transverse momentum carried by leading track: ~35% 13 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Di-jet events p T1 > 10 GeV p T2 > 10 GeV p T1 > 10 GeV p T2 > 10 GeV Di-jet asymmetry sensitive to TrackJet energy resolution nicely described in MC and detector simulation Di-jet event back-to-back in ΔФ 14 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Matching with other jet types Matching efficiency (using ΔR<0.5) 95% for p T > 40 GeV for TrackJets and CaloJets lower for p T < 40 GeV due to angular resolution of CaloJets 95% for p T > 15 GeV for TrackJets and ParticleFlowJets 15 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

TrackJets in pile-up events Example: t t µ + µ - + jets candidate event TrackJets clustered separately for each primary vertex 16 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Effect of pile-up on multi-jet events H T = Σ p T for all jets with p T >3 GeV/c in an event Vertex association eliminates pile-up effects for TrackJets Systematic effects Other systematic effects: beam background, electronic noise, mis-alignment, material budget, track quality selection: < 1% effect on TrackJets reconstruction efficiency + fake rate 17 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Analyses with TrackJets Measurement of the Underlying Event Activity (CMS PAS QCD-10-001, CMS PAS QCD-10-010) Study number and momentum of charged particles in region transverse to leading TrackJet 18 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Analyses with TrackJets Open beauty production cross section with muons (CMS PAS BPH-10-007) Transverse momentum of the muon with respect to the closest TrackJet discriminates b events from background 19 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

Conclusions TrackJets are an orthogonal approach to CaloJets in CMS used for cross-validation of jets used in analyses focusing on jet finding rather than full energy measurement TrackJets have been commissioned using 7 TeV collision data good agreement with simulation TrackJets are expected to be transparent to pile-up effects in high LHC luminosity scenarios 20 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only

References CMS PAS TRK-10-001: Tracking and Primary Vertex Results in First Collisions CMS PAS TRK-10-005: Tracking and Primary Vertex Results in First 7 TeV Collisions CMS PAS JME-08-001: Performance of Jet Reconstruction with Charged Tracks only CMS PAS JME-10-006: Commissioning of TrackJets in pp Collisions at s=7 TeV CMS PAS JME-10-003: CMS Jet Performance in pp Collisions at s=7 TeV CMS PAS QCD-10-001: First Measurement of the Underlying Event Activity in Proton-Proton Collisions at 900 GeV at the LHC CMS PAS QCD-10-010: Measurement of the Underlying Event Activity at the LHC with s = 7 TeV and Comparison with s = 0.9 TeV CMS PAS BPH-10-007: Open beauty production cross section with muons in pp collisions at s = 7 TeV 21 Andreas Hinzmann Jet Reconstruction in CMS using Charged Tracks only