Track Trigger for Taus Michael We Michael W inberger inberger and Teruki and T Kamon In collaboration with V dim Vad Va i d m i m Khotilovich

Size: px
Start display at page:

Download "Track Trigger for Taus Michael We Michael W inberger inberger and Teruki and T Kamon In collaboration with V dim Vad Va i d m i m Khotilovich"

Transcription

1 Track Trigger for Taus Michael Weinberger and Teruki Kamon In collaboration with Vadim Khotilovich and Alexei Safonov Many thanks to Laura Fields and Anders Ryd for help with their track stub code o o o o o o o OUTLINE Why taus? Phase-I Calorimeter Tau Trigger Phase-II Tracker Tau Trigger with Tracks Full Simulation Samples and Tools First Results Summary and Plan April 27,

2 Why Tau s? and Tau Trigger Physics with hadronically-decayingdeca ing taus in Higgs and SUSY Access for Z eventsents as the SM candle Calorimeter-based tau triggers at higher luminosity will be very difficult in an environment with huge QCD production cross sections with large amounts of overlapping pileup (PU) events. This requires that we will need to re-design and validate the trigger for both Phase I and II 2

3 Phase-I Calorimeter Tau Trigger Khotilovich, Mason, Safonov: Full calorimeter/muon simulation framework for simulating events in the high PU environment L1 Tau Tau(new) L1 Tau 40 GeV Tau L1 Tau(new) Trigger Rate for QCD events L1 Level 1 trigger 100 MHz Tau Tau (original config.) Tau(new) New tau trigger Tau L1 at PU50 Tau > L1 at PU100 Tau(new) degrading at PU100 We need further reduction of the trigger rate by requiring a track trigger primitive. 3

4 Phase-II Tracker Weinberger and Kamon - Full Simulation Package for Tracker (Long Barrel Geometry) - emphasis on improving tau triggering - in the SLHC Tracker Simulation Group 4

5 Stubs and Tracklets r-z view r-φφ view Stub Tracklet (vector!) 5

6 Current Long Barrel Geometry in 226 Phase 1 inner pixels In this study, the 4 th inner pixel is not included. 6

7 Tau Trigger with Tracks Assuming the matching of the seed track and a cluster can be done like in electron trigger, our focus is to test several isolation (ISO) quantities: 1) N sub =[# of stubs in ISO cone for layer k] 2) N = [# of tracklets in ISO cone] 3) I = [Σp T for tracklets in ISO cone] 4) I θ = Σ ( p T θ ) / Σp T 5)... where ISO cone = between R S and R I R S = Singnal cone radius R I = Isolation cone radius I 7

8 Full Simulation Samples and Tools (1) Full simulation package for Long Barrel Tracker (M. Weinberger) + Calorimeter (V. Khotilovich) in 226 ½ detector (to offset memory problems) (2) Test samples Ditau (p T = 10~200 GVη GeV, η = 0~2.5) + PU0 Ditau (p T = 10~200 GeV, η = 0~2.5) + PU200 [2900 events] (3) Analysis codes Laura Fields s track stub finder in 226; Clustering of stubs to remove mutiple counting not ready. Michael Mason s Phase-1 tau calo-cluster reconstruction in under migration to 226 (not fully tested yet) Today, we focus on N sub. 8

9 Hits First Look: Hits and Stubs Hit Position Stub Position y (cm m) r (cm m) η = 0 Stubs Layer Number x (cm) Stub Position z (cm) Stub Position y (cm m) Layer Number x (cm) z (cm) 9

10 First Look: Stub Rates (PU200) MHz z/cm 2 However these rates count every pixel for use in stub creation. So many stubs will be created from a single track Need clustering to remove the extra stubs Layer Number 10

11 Crude Calculation: N stub (1) Find the average rate of subs per area by layer (2) Find area of ISO cone ( θ =10 o ~ 30 o ) for a track at 45 o. (3) Combine to find the average number of stubs in the ISO cone. N stub =Area*2*Rate/40MHz 11

12 N stub in 10 o -30 o Cone one o -30 o C b in 10 o N stub Layer Number 12

13 N stub in 10 o Cone Can not compare stubs to simstubs as Fullsim does not have PU in sim path Fastsim does, so look at 50pu events and see how many stubs versus the simstubs to get estimate of overcounting Factor F t of ~10 13

14 Summary and Plan (1) We created a full simulation package for Long Barrel Tracker + Calorimeter in 226 and tested a fully simulated edsample of Ditau +PU200 events. (2) We plan to have : A full production sample of QCD events A complete analysis package Laura Fields s track stub finder in 226 Clustering to be prepared. Michael Mason s tau cluster reconstruction in migration to 226 A complete performance evaluation Isolation Track-clustermatching cuse c 14

15 Backup 15

16 Calculation: Nstub in 10o-30o Cone 16

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS NOTE 21/17 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 2 March 21 Study of a Level-3 Tau Trigger with

More information

Identifying Particle Trajectories in CMS using the Long Barrel Geometry

Identifying Particle Trajectories in CMS using the Long Barrel Geometry Identifying Particle Trajectories in CMS using the Long Barrel Geometry Angela Galvez 2010 NSF/REU Program Physics Department, University of Notre Dame Advisor: Kevin Lannon Abstract The Compact Muon Solenoid

More information

THE ATLAS TRIGGER SYSTEM UPGRADE AND PERFORMANCE IN RUN 2

THE ATLAS TRIGGER SYSTEM UPGRADE AND PERFORMANCE IN RUN 2 THE ATLAS TRIGGER SYSTEM UPGRADE AND PERFORMANCE IN RUN 2 S. Shaw a on behalf of the ATLAS Collaboration University of Manchester E-mail: a savanna.marie.shaw@cern.ch The ATLAS trigger has been used very

More information

TAMU Tau Goals at CMS

TAMU Tau Goals at CMS TAMU Tau Goals at CMS Detecting Medium- and Low-energy Tau s Proposed Plan of Work (with LPC Tau Group) A. Aurisano, M. Goncharov, A. Gurrola, T. Kamon, V. Khotilovich, C. Nguyen, J. Pivarski, A. Safonov,

More information

Reconstruction and identification of hadronic τ decays with ATLAS

Reconstruction and identification of hadronic τ decays with ATLAS Reconstruction and Identification of Hadronic τ Decays with ATLAS Wolfgang F. Mader 1 1 Institut für Kern- und Teilchenphysik TU Dresden DPG Frühjahrstagung München, March 2009 Outline 1 Introduction 2

More information

Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC

Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC Christof Roland/ MIT For the CMS Collaboration Rencontres de Moriond QCD Session 14 th March, 2010 Moriond

More information

QCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations

QCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations QCD Jets at the LHC Leonard Apanasevich University of Illinois at Chicago on behalf of the ATLAS and CMS collaborations Outline Physics at the LHC Jet Reconstruction and Performance Clustering Algorithms

More information

Triggering on Long-lived neutral particles in ATLAS

Triggering on Long-lived neutral particles in ATLAS Triggering on Long-lived neutral particles in ATLAS Our theoretical friends tell us that many extensions of the Standard Model that address the hierarchy problem contain new sectors These new sectors decouple

More information

Application of the Tau Identification Capability of CMS in the Detection of Associated Production of MSSM Heavy Neutral Higgs Bosons Souvik Das

Application of the Tau Identification Capability of CMS in the Detection of Associated Production of MSSM Heavy Neutral Higgs Bosons Souvik Das Application of the Tau Identification Capability of CMS in the Detection of Associated Production of MSSM Heavy Neutral Higgs Bosons Souvik Das Cornell University (September 11, 2006) Decays of the Tau

More information

Tau Lepton Identification at the ATLAS Experiment

Tau Lepton Identification at the ATLAS Experiment Tau Lepton Identification at the ATLAS Experiment Almut Pingel PhD Discovery Day 22 May 2012 Motivation Hadronic Tau Decay Tau ID and Pileup 2 Motivation Tau leptons are important (!!!). Higgs searches

More information

The ATLAS C. Gemme, F.Parodi

The ATLAS C. Gemme, F.Parodi The ATLAS Experiment@LHC C. Gemme, F.Parodi LHC physics test the Standard Model, hopefully find physics beyond SM find clues to the EWK symmetry breaking - Higgs(ses)? Standard Model is a gauge theory

More information

Physics potential of ATLAS upgrades at HL-LHC

Physics potential of ATLAS upgrades at HL-LHC M.Testa on behalf of the ATLAS Collaboration INFN LNF, Italy E-mail: marianna.testa@lnf.infn.it ATL-PHYS-PROC-207-50 22 September 207 The High Luminosity-Large Hadron Collider (HL-LHC) is expected to start

More information

EGAMMA HLT. Marco Pieri. UCSD Meeting 12 June 2007

EGAMMA HLT. Marco Pieri. UCSD Meeting 12 June 2007 EGAMMA HLT Marco Pieri UCSD Meeting 12 June 2007 Introduction For low luminosity 2x10 33 cm -2 s -1 : We assume a Level1 trigger rate of 50 khz We apply a safety factor of 3 and set the L1 rate at 17 khz

More information

The rejection of background to the H γγ process using isolation criteria based on information from the electromagnetic calorimeter and tracker.

The rejection of background to the H γγ process using isolation criteria based on information from the electromagnetic calorimeter and tracker. Available on CMS information server CMS NOTE 22/3 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland September 9, 22 The rejection of background to

More information

Future prospects for the measurement of direct photons at the LHC

Future prospects for the measurement of direct photons at the LHC Future prospects for the measurement of direct photons at the LHC David Joffe on behalf of the and CMS Collaborations Southern Methodist University Department of Physics, 75275 Dallas, Texas, USA DOI:

More information

PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2

PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2 PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2 M.M. Morgenstern On behalf of the ATLAS collaboration Nikhef, National institute for subatomic physics, Amsterdam, The Netherlands E-mail: a marcus.matthias.morgenstern@cern.ch

More information

HL-LHC Physics with CMS Paolo Giacomelli (INFN Bologna) Plenary ECFA meeting Friday, November 23rd, 2012

HL-LHC Physics with CMS Paolo Giacomelli (INFN Bologna) Plenary ECFA meeting Friday, November 23rd, 2012 @ HL-LHC Physics with CMS Paolo Giacomelli (INFN Bologna) Plenary ECFA meeting Friday, November 23rd, 2012 Many thanks to several colleagues, in particular: M. Klute and J. Varela Outline Where we stand

More information

ATLAS-CONF October 15, 2010

ATLAS-CONF October 15, 2010 ATLAS-CONF-2010-096 October 15, 2010 Data-driven background estimation for the H τ + τ τ h search at 7 TeV with the ATLAS detector Ian Howley 7 December 2010 1 Motivation One of the primary LHC physics

More information

ATLAS Calorimetry (Geant)

ATLAS Calorimetry (Geant) signature for New Physics (e.g. compositness, jet multiplicity in SUSY) high of E miss in LHC physics: Importance used in invariant mass reconstruction in decays neutrinos: A=H! fifi, t! lνb, etc. involving

More information

Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV

Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV EDSBlois 2015 02.07.2015 Dominik Haitz on behalf of the ATLAS and CMS Collaborations INSTITUT FÜR EXPERIMENTELLE KERNPHYSIK

More information

Alignment of the ATLAS Inner Detector

Alignment of the ATLAS Inner Detector Alignment of the ATLAS Inner Detector Roland Härtel - MPI für Physik on behalf of the ATLAS inner detector alignment group Outline: LHC / ATLAS / Inner Detector Alignment approaches Results Large Hadron

More information

Walter Hopkins. February

Walter Hopkins. February B s µ + µ Walter Hopkins Cornell University February 25 2010 Walter Hopkins (Cornell University) Bs µ + µ February 25 2010 1 / 14 Motivation B s µ + µ can only occur through higher order diagrams in Standard

More information

Di muons and the detection of J/psi, Upsilon and Z 0 Jets and the phenomenon of jet quenching

Di muons and the detection of J/psi, Upsilon and Z 0 Jets and the phenomenon of jet quenching collisions in CMS Bolek Wyslouch École Polytechnique Massachusetts Institute of Technology on behalf of CMS Collaboration CERN, December 2, 2010 1 Heavy Ions at the LHC Huge energy jump from RHIC: factor

More information

Design of the new ATLAS Inner Tracker for the High Luminosity LHC era

Design of the new ATLAS Inner Tracker for the High Luminosity LHC era Design of the new ATLAS Inner Tracker for the High Luminosity LHC era Trevor Vickey on behalf of the ATLAS Collaboration University of Sheffield, United Kingdom July 3, 2017 19th iworid Krakow, Poland

More information

CMS Trigger Simulation

CMS Trigger Simulation CMS Trigger Simulation Sridhara Dasu University of Wisconsin Outline: Calorimeter Level- Trigger Algorithms Rates and Efficiencies Physics Performance Muon Level- Trigger Algorithms Rates and Efficiencies

More information

Atlas Status and Perspectives

Atlas Status and Perspectives Atlas Status and Perspectives Bruno Mansoulié (IRFU-Saclay) On behalf of the Topics The hot news: Heavy Ion analysis Data taking in 2010 Luminosity, Data taking & quality, trigger Detector performance

More information

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS NOTE 22/? The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-2 GENEVA 23, Switzerland xxxx Study of a High Level b-trigger selection of

More information

QCD at the Tevatron: The Production of Jets & Photons plus Jets

QCD at the Tevatron: The Production of Jets & Photons plus Jets QCD at the Tevatron: The Production of Jets & Photons plus Jets Mike Strauss The University of Oklahoma The Oklahoma Center for High Energy Physics for the CDF and DØD Collaborations APS 2009 Denver, Colorado

More information

Risultati dell esperimento ATLAS dopo il run 1 di LHC. C. Gemme (INFN Genova), F. Parodi (INFN/University Genova) Genova, 28 Maggio 2013

Risultati dell esperimento ATLAS dopo il run 1 di LHC. C. Gemme (INFN Genova), F. Parodi (INFN/University Genova) Genova, 28 Maggio 2013 Risultati dell esperimento ATLAS dopo il run 1 di LHC C. Gemme (INFN Genova), F. Parodi (INFN/University Genova) Genova, 28 Maggio 2013 1 LHC physics Standard Model is a gauge theory based on the following

More information

Searches using displaced leptons or jets

Searches using displaced leptons or jets Searches using displaced leptons or jets J Antonelli with input from M Flowerdew, P Pais, R Rosten, H Russell I ve spoken with authors from ~all of the relevant searches, here are some general musings

More information

Physics with Jets at the LHC

Physics with Jets at the LHC XXXIV Int. Symp. on Multiparticle Dynamics, Sonoma County, July 29, 2004 ISMD Rohlf p.1/50 Physics with Jets at the LHC Jim Rohlf Boston University Outline Introduction Detectors and expected performance

More information

Electroweak Physics at the Tevatron

Electroweak Physics at the Tevatron Electroweak Physics at the Tevatron Adam Lyon / Fermilab for the DØ and CDF collaborations 15 th Topical Conference on Hadron Collider Physics June 2004 Outline Importance Methodology Single Boson Measurements

More information

Study of Quark compositeness in pp q * at CMS

Study of Quark compositeness in pp q * at CMS Study of Quark compositeness in pp q * at CMS + Jets Brajesh Choudhary, Debajyoti Choudhury, Varun Sharma University of Delhi, Delhi Sushil Singh Chauhan, Mani Tripathi University of California, Davis

More information

The ATLAS muon and tau triggers

The ATLAS muon and tau triggers Journal of Physics: Conference Series OPEN ACCESS The ATLAS muon and tau triggers To cite this article: L Dell'Asta and the Atlas Collaboration 2014 J. Phys.: Conf. Ser. 523 012018 View the article online

More information

Introduction. Tau leptons. SLHC. Summary. Muons. Scott S. Snyder Brookhaven National Laboratory ILC Physics and Detector workshop Snowmass, Aug 2005

Introduction. Tau leptons. SLHC. Summary. Muons. Scott S. Snyder Brookhaven National Laboratory ILC Physics and Detector workshop Snowmass, Aug 2005 Leptons and Photons at the (S)LHC Scott S. Snyder Brookhaven National Laboratory ILC Physics and Detector workshop Snowmass, Aug 2005 Outline: Introduction. e/γ. Muons. Tau leptons. SLHC. Summary. Leptons

More information

Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC

Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC Matthias Hamer on behalf of the ATLAS collaboration Introduction The ATLAS Phase II Inner Tracker Expected Tracking Performance

More information

Nikos Varelas. University of Illinois at Chicago. CTEQ Collaboration Meeting Northwestern November 20, Nikos Varelas. CTEQ Meeting Nov 20, 2009

Nikos Varelas. University of Illinois at Chicago. CTEQ Collaboration Meeting Northwestern November 20, Nikos Varelas. CTEQ Meeting Nov 20, 2009 QCD Physics at CMS University of Illinois at Chicago CTEQ Collaboration Meeting Northwestern November 0, 009 1 QCD Physics at CMS University of Illinois at Chicago CTEQ Collaboration Meeting Northwestern

More information

Upgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential

Upgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential IL NUOVO CIMENTO 4 C (27) 8 DOI.393/ncc/i27-78-7 Colloquia: IFAE 26 Upgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential M. Testa LNF-INFN - Frascati (RM), Italy

More information

PoS(EPS-HEP 2013)508. CMS Detector: Performance Results. Speaker. I. Redondo * CIEMAT

PoS(EPS-HEP 2013)508. CMS Detector: Performance Results. Speaker. I. Redondo * CIEMAT : Performance Results * CIEMAT Av. Compluense 40 Madrid 28040, Spain E-mail: ignacio.redondo@ciemat.es The Compact Muon Solenoid (CMS) detector is one of the two multipurpose experiments at the Large Hadron

More information

The ATLAS trigger - commissioning with cosmic rays

The ATLAS trigger - commissioning with cosmic rays Journal of Physics: Conference Series The ATLAS trigger - commissioning with cosmic rays To cite this article: J Boyd 2008 J. Phys.: Conf. Ser. 119 022014 Related content - The ATLAS Level-1 Central Trigger

More information

PoS(ICHEP2012)049. Study of tau-pair production at HERA. Masaki Ishitsuka Tokyo Institute of Technology

PoS(ICHEP2012)049. Study of tau-pair production at HERA. Masaki Ishitsuka Tokyo Institute of Technology Tokyo Institute of Technology E-mail: ishitsuka@phys.titech.ac.jp for ZEUS Collaboration A study of tau-pair production has been performed with the ZEUS detector at HERA ep collider, using a data sample

More information

Recent Results from 7 GeV proton proton running at CMS

Recent Results from 7 GeV proton proton running at CMS Recent Results from 7 GeV proton proton running at CMS Will E. Johns Vanderbilt University (for the CMS collaboration) SESAPS 2011 CMS Detector Detector pulled Apart for work 2 CMS Detector CMS Detector

More information

The ATLAS Detector - Inside Out Julia I. Hofmann

The ATLAS Detector - Inside Out Julia I. Hofmann The ATLAS Detector - Inside Out Julia I. Hofmann KIP Heidelberg University Outline: 1st lecture: The Detector 2nd lecture: The Trigger 3rd lecture: The Analysis (mine) Motivation Physics Goals: Study Standard

More information

Muon reconstruction performance in ATLAS at Run-2

Muon reconstruction performance in ATLAS at Run-2 2 Muon reconstruction performance in ATLAS at Run-2 Hannah Herde on behalf of the ATLAS Collaboration Brandeis University (US) E-mail: hannah.herde@cern.ch ATL-PHYS-PROC-205-2 5 October 205 The ATLAS muon

More information

Long lived particle decay LHC. Simone Gennai on behalf of the ATLAS, CMS and LHCb Collaborations

Long lived particle decay LHC. Simone Gennai on behalf of the ATLAS, CMS and LHCb Collaborations Long lived particle decay searches @ LHC Simone Gennai on behalf of the ATLAS, CMS and LHCb Collaborations 1 Why searching for LLP? 2 Standard Model includes quite few LLP it is natural to assume they

More information

Electron reconstruction and identification in CMS at LHC

Electron reconstruction and identification in CMS at LHC Electron reconstruction and identification in CMS at LHC on behalf of CMS collaboration 1 Outline The CMS detector @ LHC Electron reconstruction components Performance Electron identification Measurements

More information

Reconstruction of tau leptons and prospects for SUSY in ATLAS. Carolin Zendler University of Bonn for the ATLAS collaboration

Reconstruction of tau leptons and prospects for SUSY in ATLAS. Carolin Zendler University of Bonn for the ATLAS collaboration Reconstruction of tau leptons and prospects for SUSY in ATLAS Carolin Zendler University of Bonn for the ATLAS collaboration SUSY09, Boston 05.06.-10.06. 2009 Outline I Introduction and Motivation II Tau

More information

Charged Particle Production in Pb+Pb Collisions at snn=2.76 TeV with the ATLAS detector at the LHC

Charged Particle Production in Pb+Pb Collisions at snn=2.76 TeV with the ATLAS detector at the LHC Charged Particle Production in Pb+Pb Collisions at snn=2.76 TeV with the ATLAS detector at the LHC Dominik Derendarz for the ATLAS Collaboration Institute of Nuclear Physics PAN, Kraków, Poland Introduction

More information

Seaches fo log-lived paticles with displaced signatues at the LHC. Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations

Seaches fo log-lived paticles with displaced signatues at the LHC. Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations Seaches fo log-lived paticles with displaced signatues at the LHC Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations Outline A review of the most recent results from ATLAS &

More information

A Update on Electron Isolation

A Update on Electron Isolation A Update on Electron Isolation Matthew LeBourgeois Vivek Sharma UCSD Group Meeting 5th February, 2008 Table of Contents To date, have shown muon isolation studies http://indico.cern.ch/getfile.py/access?contribid=8&resid=0&materialid=slides&confid=20377

More information

Inclusive SUSY Searches at CMS with Emphasis on Detector Systematics

Inclusive SUSY Searches at CMS with Emphasis on Detector Systematics Inclusive SUSY Searches at with Emphasis on Detector Systematics R. Cavanaugh (on behalf of ) University of Florida SUSY06 Detector Background Calibrations Inclusive Search Strategies Detector Systematics

More information

FATRAS. A Novel Fast Track Simulation Engine for the ATLAS Experiment. Sebastian Fleischmann on behalf of the ATLAS Collaboration

FATRAS. A Novel Fast Track Simulation Engine for the ATLAS Experiment. Sebastian Fleischmann on behalf of the ATLAS Collaboration A Novel Fast Track Engine for the ATLAS Experiment on behalf of the ATLAS Collaboration Physikalisches Institut University of Bonn February 26th 2010 ACAT 2010 Jaipur, India 1 The ATLAS detector Fast detector

More information

Upgrade of ATLAS Electron and Photon Triggers and Performance for LHC Run2

Upgrade of ATLAS Electron and Photon Triggers and Performance for LHC Run2 Upgrade of ALAS Electron and Photon riggers and Performance for LHC Run2 Ryan Mackenzie White (UFSM,Chile) on behalf of ALAS Collaboration NEC 2015 XXV International Symposium on Nuclear Electronics &

More information

Preparations for the ATLAS Heavy Ion Physics Program at the LHC. Deepak Kar IKTP, TU Dresden On behalf of the ATLAS Collaboration

Preparations for the ATLAS Heavy Ion Physics Program at the LHC. Deepak Kar IKTP, TU Dresden On behalf of the ATLAS Collaboration Preparations for the ATLAS Heavy Ion Physics Program at the LHC Deepak Kar IKTP, TU Dresden On behalf of the ATLAS Collaboration 1 QCD Hadronic phase: Bound states of quark and gluon pp collisions Heavy

More information

ATLAS muon reconstruction efficiency with a tag & probe technique on Z boson dimuon decay

ATLAS muon reconstruction efficiency with a tag & probe technique on Z boson dimuon decay ATLAS muon reconstruction efficiency with a tag & probe technique on Z boson dimuon decay ------Alessandro Manfredini-----Muon Combined Performance group (Roma Tre University) Talk structure: Introduction:

More information

A Search for Doubly Charged Higgs Production at 8 TeV Using the CMS Detector at the LHC

A Search for Doubly Charged Higgs Production at 8 TeV Using the CMS Detector at the LHC A Search for Doubly Charged Higgs Production at 8 TeV Using the CMS Detector at the LHC 1 UW-Madison Preliminary Examination Outline The Standard Model Doubly Charged Higgs Motivation Type II Seesaw Mechanism

More information

Light Charged Higgs Discovery Potential of CMS in. A. Nikitenko, M. Hashemi, Imperial College, IPM & Sharif Univ. of Tech.

Light Charged Higgs Discovery Potential of CMS in. A. Nikitenko, M. Hashemi, Imperial College, IPM & Sharif Univ. of Tech. Light Charged Higgs Discovery Potential of CMS in the H ± τν Decay A. Nikitenko, M. Hashemi, Imperial College, IPM & Sharif Univ. of Tech. London Tehran Outline: Signal and background identification Signal

More information

Searches for Long-Lived Particles in ATLAS: challenges and opportunities of HL-LHC

Searches for Long-Lived Particles in ATLAS: challenges and opportunities of HL-LHC Searches for Long-Lived Particles in ATLAS: challenges and opportunities of HL-LHC Simone Pagan Griso Lawrence Berkeley National Lab. on behalf of the ATLAS Collaboration HL(/HE)-LHC Yellow-Report kick-off

More information

Collider Physics Analysis Procedures

Collider Physics Analysis Procedures Collider Physics Analysis Procedures Alex Tapper Slides available at: http://www.hep.ph.ic.ac.uk/~tapper/lecture.html Aim Overview of analysis techniques at CMS Contrast with Tevatron (see DØ lecture)

More information

First V+jets results with CMS. Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8-10 Sep 2010, Durham

First V+jets results with CMS. Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8-10 Sep 2010, Durham First V+jets results with CMS Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8- Sep 20, Durham Outline Jet and missing energy reconstruction W and Z selections and cross-section measurement First

More information

Search for long-lived particles at CMS. TeVPA Brian Francis for the CMS Collaboration

Search for long-lived particles at CMS. TeVPA Brian Francis for the CMS Collaboration Search for long-lived particles at CMS TeVPA 7 Brian Francis for the CMS Collaboration Long-lived particles (LLP) at CMS Despite best efforts, no evidence yet of BSM physics at the LHC If it s not where

More information

Rare B decays in ATLAS and CMS

Rare B decays in ATLAS and CMS Rare B decays in ATLAS and CMS University Dec. 14 th 2006 Makoto Tomoto Nagoya University on behalf of CMS and ATLAS collaborations Makoto Tomoto (Nagoya University) Outline B physics in ATLAS and CMS

More information

Electron Isolation Performance

Electron Isolation Performance Electron Isolation Performance LeBourgeois, Matthew 13th November, 2007 Table of Contents To date, have only shown muon isolation studies http://indico.cern.ch/getfile.py/access?contribid=8&resid=0&materialid=slides&confid=20377

More information

Analysis of a Potential Tracking Algorithm for the SLHC Upgrade

Analysis of a Potential Tracking Algorithm for the SLHC Upgrade Analysis of a Potential Tracking Algorithm for the SLHC Upgrade Rachael Creager Michael Swift 2012 NSF/REU Program Physics Department, University of Notre Dame Advisors: Professor Michael Hildreth Professor

More information

The HL-LHC physics program

The HL-LHC physics program 2013/12/16 Workshop on Future High Energy Circular Collider 1 The HL-LHC physics program Takanori Kono (KEK/Ochanomizu University) for the ATLAS & CMS Collaborations Workshop on Future High Energy Circular

More information

Introduction on ATLAS FCPPL Project ACC/CEA/IN2P3. Emmanuel MONNIER (CPPM)

Introduction on ATLAS FCPPL Project ACC/CEA/IN2P3. Emmanuel MONNIER (CPPM) Introduction on ATLAS FCPPL Project ACC/CEA/IN2P3 Emmanuel MONNIER (CPPM) FCPPL 5 th workshop 21 March 2012 1 p T (e) = 64 GeV, E T Miss = 21 GeV p T (μ + ) = 65 GeV, p T (μ - ) = 40 GeV M T = 57 GeV,

More information

Lepton and Photon reconstruction and identification performance in CMS and ATLAS

Lepton and Photon reconstruction and identification performance in CMS and ATLAS Lepton and Photon reconstruction and identification performance in CMS and ATLAS Sandro Fonseca de Souza, on behalf of the CMS and ATLAS Collaborations Universidade do Estado do Rio de Janeiro Large Hadron

More information

The Heavy Quark Search at the LHC

The Heavy Quark Search at the LHC The Heavy Quark Search at the LHC The Heavy Quark Search at the LHC Backgrounds: estimating and suppressing tt, multijets,... jet mass technique NLO effects matrix elements for extra jets initial state

More information

CMS Trigger Simulation Sridhara Dasu University of Wisconsin

CMS Trigger Simulation Sridhara Dasu University of Wisconsin CMS Trigger Simulation Sridhara Dasu University of Wisconsin Outline: Calorimeter Level- Trigger Algorithms Rates and Efficiencies Muon Level- Trigger Algorithms Rates and Efficiencies Combined Rates Physics

More information

Prospect for WW Study with Early ATLAS Data

Prospect for WW Study with Early ATLAS Data Prospect for WW Study with Early ATLAS Data N. Vranješ, Lj. Simić, D.S.Popović ATLAS@Institute of Physics Motivation and WW production at LHC Event reconstruction and selection WW production measurement

More information

Jet fragmentation study in vacuum and in medium in the ALICE experiment at the LHC

Jet fragmentation study in vacuum and in medium in the ALICE experiment at the LHC Jet fragmentation study in vacuum and in medium in the ALICE experiment at the LHC Magali Estienne for the ALICE Collaboration WISH 2010 Catania, Italia, September 8-10 2010 Outline 2 Motivations for jet

More information

CMS: Muon System and Physics performance

CMS: Muon System and Physics performance VI symposium on LHC Physics and Detectors Fermilab, Batavia, Il, U.S., may, 2003 CMS: Muon System and Physics performance Stefano Lacaprara, I.N.F.N. and Padova University on behalf of the CMS collaboration

More information

Analysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments

Analysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments Analysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments In Collaboration with Manuel Drees August 23rd, 2010 SUSY10 1 Introduction 2 Ghost Events 3 Simulation 4 Outlook and Summary Introduction

More information

Top Physics in Hadron Collisions

Top Physics in Hadron Collisions Top Physics in Hadron Collisions Dirk Dammann DESY 2010-02-04 1 / 44 Outline 1 2 3 4 2 / 44 Outline Motivation Top Production Top Decay Top Physics 1 Motivation Top Production Top Decay Top Physics 2 3

More information

Commissioning of the CMS Detector

Commissioning of the CMS Detector Commissioning of the CMS Detector Marina Giunta INFN Bologna On behalf of the CMS Collaboration XLIVth Rencontres de Moriond on QCD and High Energy Interactions La Thuile,14-21 March 2009 2008: very busy

More information

Higgs-related SM Measurements at ATLAS

Higgs-related SM Measurements at ATLAS Higgs-related SM Measurements at ATLAS Junjie Zhu University of Michigan 2 nd MCTP Spring Symposium on Higgs Boson Physics Outline Introduction Isolated γγ cross section (37 pb -1, Phys. Rev. D 85, 012003

More information

Performance of muon and tau identification at ATLAS

Performance of muon and tau identification at ATLAS ATL-PHYS-PROC-22-3 22/2/22 Performance of muon and tau identification at ATLAS On behalf of the ATLAS Collaboration University of Oregon E-mail: mansoora.shamim@cern.ch Charged leptons play an important

More information

Early physics with Atlas at LHC

Early physics with Atlas at LHC Early physics with Atlas at LHC Bellisario Esposito (INFN-Frascati) On behalf of the Atlas Collaboration Outline Atlas Experiment Physics goals Next LHC run conditions Physics processes observable with

More information

Ridge correlation structure in high multiplicity pp collisions with CMS

Ridge correlation structure in high multiplicity pp collisions with CMS Ridge correlation structure in high multiplicity pp collisions with CMS Dragos Velicanu for the CMS Collaboration MBUEWG CERN, Geneva, June 17 2011 Results from High Multiplicity pp Dragos Velicanu (MIT)

More information

Christian Wiel. Reconstruction and Identification of Semi-Leptonic Di-Tau Decays in Boosted Topologies at ATLAS

Christian Wiel. Reconstruction and Identification of Semi-Leptonic Di-Tau Decays in Boosted Topologies at ATLAS 22.3.8 / 6 Reconstruction and Identification of Semi-Leptonic Di-Tau Decays in Boosted Topologies at ATLAS 22.3.8 2 / 6 Tau Lepton Properties 8% 7% other 6% 4% 35% leptonic % 9% 65% hadronic 9% 25% 22.3.8

More information

7 Physics at Hadron Colliders

7 Physics at Hadron Colliders 7 Physics at Hadron Colliders The present and future Hadron Colliders - The Tevatron and the LHC Test of the Standard Model at Hadron Colliders Jet, W/Z, Top-quark production Physics of Beauty Quarks (T.

More information

CMS Searches for SUSY in Hadronic Final States

CMS Searches for SUSY in Hadronic Final States CMS Searches for SUSY in Hadronic Final States Teruki Kamon on behalf of the CMS Collaboration Mitchell Institute for Fundamental Physics and Astronomy Texas A&M University JnHF 2018: Santa Fe Jets and

More information

Jet reconstruction with first data in ATLAS

Jet reconstruction with first data in ATLAS University of Victoria, Victoria, BC, Canada E-mail: damir.lelas@cern.ch The algorithms used for jet reconstruction in ATLAS are presented. General performance aspects like jet signal linearity and the

More information

Pileup measurement and mitigation techniques in CMS

Pileup measurement and mitigation techniques in CMS Pileup measurement and mitigation techniques in CMS A Perloff, on behalf of the CMS collaboration Graduate Student, Department of Physics and Astronomy, exas A&M University, College Station, X 7784-44,

More information

Efficient Implementation of High- Energy Physics Processing Using Modified Jet Reconstruction and Active Size Partitioning

Efficient Implementation of High- Energy Physics Processing Using Modified Jet Reconstruction and Active Size Partitioning Efficient Implementation of High- Energy Physics Processing Using Modified Jet Reconstruction and Active Size Partitioning Tony Gregerson University of Wisconsin Tony Gregerson, U. Wisconsin, 13 April

More information

ATLAS Run 2 Higgs Prospects

ATLAS Run 2 Higgs Prospects ATLAS Run 2 Higgs Prospects Jessica Levêque LAPP Annecy-le-Vieux CNRS/IN2P3 on behalf of The ATLAS Collaboration Outline ATLAS Upgrades during LS1 ATLAS readiness First physics results with Run 2 data

More information

A Toroidal LHC ApparatuS

A Toroidal LHC ApparatuS Status of ATLAS A Toroidal LHC ApparatuS V 1.0 Frank Taylor MIT Fourth ATLAS Physics Workshop of the Americas August 9 11, 2010 University of Texas, Arlington, TX We Americans of ATLAS Argentina, Brazil,

More information

Tau Performance. ATLAS UK Physics Meeting. Alan Phillips University of Cambridge. ( on behalf of the Tau Working Group)

Tau Performance. ATLAS UK Physics Meeting. Alan Phillips University of Cambridge. ( on behalf of the Tau Working Group) Tau Performance ATLAS UK Physics Meeting 9 th January 2008 Alan Phillips University of Cambridge ( on behalf of the Tau Working Group) 1 Overview I plan to cover the following topics as a sample of the

More information

The LHCb Upgrade. On behalf of the LHCb Collaboration. Tomasz Szumlak AGH-UST

The LHCb Upgrade. On behalf of the LHCb Collaboration. Tomasz Szumlak AGH-UST The LHCb Upgrade Outline LHCb Detector Selected Physics Results Upgrade Plans Test beam campaign (just a flash) Summary On behalf of the LHCb Collaboration Tomasz Szumlak AGH-UST 1 XII International Conference

More information

The Compact Muon Solenoid Experiment. CMS Note. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. R. Kinnunen

The Compact Muon Solenoid Experiment. CMS Note. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. R. Kinnunen Available on CMS information server CMS NOE 2003/006 he Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 24 March 2003 Study of H ττ with hadronic τ decays

More information

Physics with Tau Lepton Final States in ATLAS. Felix Friedrich on behalf of the ATLAS Collaboration

Physics with Tau Lepton Final States in ATLAS. Felix Friedrich on behalf of the ATLAS Collaboration Physics with Tau Lepton Final States in ATLAS on behalf of the ATLAS Collaboration HEP 2012, Valparaiso (Chile), 06.01.2012 The Tau Lepton m τ = 1.8 GeV, heaviest lepton cτ = 87 μm, short lifetime hadronic

More information

Measurement of charged particle spectra in pp collisions at CMS

Measurement of charged particle spectra in pp collisions at CMS Measurement of arged particle spectra in pp collisions at CMS for the CMS Collaboration Eötvös Loránd University, Budapest, Hungary E-mail: krisztian.krajczar@cern. We present the plans of the CMS collaboration

More information

The ATLAS Run 2 Trigger: Design, Menu, Performance and Operational Aspects

The ATLAS Run 2 Trigger: Design, Menu, Performance and Operational Aspects he ALAS Run rigger: Design, Menu, Performance and Operational Aspects, on behalf of the ALAS Collaboration University of Pennsylvania E-mail: jmiguens@cern.ch AL-DAQ-PROC-6-5 5//6 he LHC, at design capacity,

More information

First physics with the ATLAS and CMS experiments. Niels van Eldik on behalf of the ATLAS and CMS collaborations

First physics with the ATLAS and CMS experiments. Niels van Eldik on behalf of the ATLAS and CMS collaborations First physics with the ATLAS and CMS experiments Niels van Eldik on behalf of the ATLAS and CMS collaborations Content Status of the LHC and the ATLAS and CMS experiments Event production rates First physics

More information

Alexei Safonov Lecture #18

Alexei Safonov Lecture #18 Methods of Experimental Particle Physics Alexei Safonov Lecture #18 1 Presentations: Trigger Today Lecture D0 calorimeter by Jeff 2 Collisions at LHC 14 000 x mass of proton (14 TeV) = Collision Energy

More information

LHC Searches for Neutrino Physics in t Channel Heavy Neutrino, Z and W

LHC Searches for Neutrino Physics in t Channel Heavy Neutrino, Z and W LHC Searches for Neutrino Physics in t Channel Heavy Neutrino, Z and W Teruki Kamon Mitchell Institute for Fundamental Physics and Astronomy Texas A&M University Workshop on "Neutrinos at the High Energy

More information

Physics at Hadron Colliders

Physics at Hadron Colliders Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD

More information

THE MULTIPLICIY JUMP! FINDING B S IN MULTI-TEV JETS W/O TRACKS

THE MULTIPLICIY JUMP! FINDING B S IN MULTI-TEV JETS W/O TRACKS 1 THE MULTIPLICIY JUMP! FINDING B S IN MULTI-TEV JETS W/O TRACKS TODD HUFFMAN, OXFORD UNIVERSITY THOMAS RUSSELL, CURRENTLY @ BLOOMBERG L.P. JEFF TSENG, OXFORD UNIVERSITY ARXIV:1701.06832 ALSO: 2016 J.PHYS.

More information

Motivations for a L1 Track Trigger

Motivations for a L1 Track Trigger Motivations for a L1 Track Trigger Véronique Boisvert, RHUL TDAQ week Rome May 2009 Thanks to: Simon G., Alan W., Monika W., Stefan T., Fred W., Pedro T., Teresa F., Michael B. Motivation for the Motivation

More information

Track Reconstruction in Hadronic Tau Decays at the ATLAS Detector

Track Reconstruction in Hadronic Tau Decays at the ATLAS Detector rack Reconstruction in Hadronic au Decays at the ALAS Detector Dirk Duschinger DPG Fruehjahrstagung Wuppertal March 9, 25 Dirk Duschinger (dirk.duschinger@cern.ch) rack Reconstruction in Hadronic au Decays

More information