ATLAS HLT Steering. Andrey Belkin Johannes Gutenberg Universität Mainz

Size: px
Start display at page:

Download "ATLAS HLT Steering. Andrey Belkin Johannes Gutenberg Universität Mainz"

Transcription

1 ATLAS HLT Steering Johannes Gutenberg Universität Mainz 36. Herbstschule für Hochenergiephysik Maria Laach,

2 Overview ATLAS detector Trigger system Steering Performance tests Status and outlook Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 2

3 Physical peculiarities High collision rate: about 40MHz Strong reduction of data rate is needed Background: one physically interesting Event in up to 10 8 Events The Trigger System must be very effective Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 3

4 LHC / ATLAS detector Large Hadron Collider (LHC): p-p Storage Ring at CERN (Geneva), center of mass energy s=14tev, length 26,6 km, design luminosity /(cm 2 s), collision rate 40 MHz ATLAS detector: Angle acceptance ~4π, data channels O(10 8 ), length 40m, height 22m, weight 7000t Muon detectors ( η <2,7) Solenoid magnets (2T) Toroid magnets Main goals: Higgs-Bosons New physics (e.g. SUSY) Electromagnetic calorimeter ( η <5) Hadronic calorimeter ( η <5) Inner detector (Silicon-pixel, -strip Detektoren, Transition Radiation Tracker) Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 4

5 Calorimetry hadronic calorimeter e.m. calorimeter e.m. (e, γ) hadron Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 5

6 Space angles and granularity η = -ln tan(θ/2) Data: isolated traces on e.m./had planes, calorimeter values, tracks, etc. Isolation: a tower upon two calorimeter levels (e.m., had), slides and seeks isolated elements We need to reconstruct the event by given data The main data reduction at the first step is in Regions of Interest concept Areas selected by Trigger - Regions of Interest (RoIs) Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 6

7 Trigger system The idea of three-stage architecture: reject highrated background processes at the earliest possible time leaving complex and slow algorithms for the latest steps. For example, Lvl-1 reduces data of Event to RoIs, Lvl-2 applies calorimeter data, EF applies track and isolation data High-rate process selection in three stages: Level-1 - Data from Calorimeter trigger (analog energy sums from calorimeter cells Δη Δϕ = ), Muon trigger, RoIs, etc. - Trigger decisions within maximum 2 µs Hardware/Firmware implementation - Event rate must be reduced from 40 MHz to khz H L T HLT: Level-2, Event Filter (my part) - Event rate must be reduced from 75 khz to 1-2 khz and then to Hz - Trigger decisions within maximum 1 ms-1 sec Software implementation on a computer farm - Reconstruction and selection of Events Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 7

8 Steering In order to reconstruct the Event we need to apply algorithms that combine all gathered by LVL1 data (energy, RoI, track, etc.) and test if it is physically interesting one For this, the HLT implements Steering, which is a mechanism to drive running of algorithms in certain sequences for classifying and selecting Events according to given schema Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 8

9 EMTAUROI MUONROI HLT workflow tau_cand? g_cand? e_cand? Example: electron reconstruction, at the end we are interested in finding one isolated electron of energy at least 25 GeV In the schema of interesting Events we specify e25i From the LVL1 we receive different RoIs, like EMTAUROI, MUONROI, JETROI, etc. In principle, we need to define in reconstruction sequence that EMTAUROI leads to creation of three hypotheses: tau_cand, g_cand, e_cand The hypotheses are created and passed by Steering to corresponding algorithms that approve or decline them, like L2Alg_ApprECand( ) If the hypothesis is approved the Steering looks into the reconstruction sequence for next hypotheses and algorithms, like e25_calo, e60_calo to EFAlg_ApplyCalo( ), then track and isolation processing If all hypotheses were successful, at the end we will approve the e25i hypothesis and then the Steering will report the match to the schema element e25i and will save the Event Steering L2Alg_ApprECand(...) e_cand! e25_calo? e60_calo?... Steering Schema: e25i... Steering Success! Save Event Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p EFAlg_ApplyCalo(...) e25_calo!... e25i!...

10 Processing buffer (StoreGate) We operate with different objects, like energy, RoIs, etc. This objects are linked to corresponding hypothesis that is just a label, like e25_calo, e25i When the hypothesis is passed to processing, the algorithm retrieves the physical data from storage by hypothesis label Hypotheses and objects are linked together with uses, excludes, seeded by relationships We can navigate through the tree of linked objects in order to obtain all data of each hypothesis Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 10

11 Processing of trigger objects tree EMTAUROI uses Object of EMTauRoi class seeded by tau_cand excludes e_cand g_cand e_cand excludes g_cand tau_cand g_cand excludes e_cand tau_cand Receive input hypothesis Algorithm Navigate through the tree and process data, attach new objects Approve input hypothesis to activate it and initiate the creation of a new hypothesis Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 11

12 Sequences of algorithms and the Menu Sequences <SEQUENCE level="l2" input="emtauroi" algorithm="l2alg_roi2cand/roi2cand/roi2cand" output="e_cand" /> <SEQUENCE level="ef" input="e_cand" algorithm="efalg_cand2calo/cand2calo/cand2calo" output="e25_calo" /> <SEQUENCE level="ef" input="e25_calo" algorithm="efalg_calo2track/calo2track/calo2track" output="e25_track" /> <SEQUENCE level="ef" input="e25_track" algorithm="efalg_track2result/track2result/track2result" output="e25i" /> <SEQUENCE level="ef" input="e_cand" algorithm="efalg_cand2calo/cand2calo/cand2calo" output="e15_calo" /> <SEQUENCE level="ef" input="e15_calo" algorithm="efalg_calo2track/calo2track/calo2track" output="e15_track" /> <SEQUENCE level="ef" input="e15_track" algorithm="efalg_track2result/track2result/track2result" output="e15i" /> Menu <SIGNATURE signature_id="e25i" prescale="1" forced_accept="0"> <TRIGGERELEMENT te_name="e25i" /> </SIGNATURE> <SIGNATURE signature_id="e15ix2" prescale="1" forced_accept="0"> <TRIGGERELEMENT te_name="e15i" /> <TRIGGERELEMENT te_name="e15i" /> </SIGNATURE> Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 12

13 joboption ApplicationMgr.DLLs += { "GaudiAud" }; AuditorSvc.Auditors += { "ChronoAuditor" }; AuditorSvc.Auditors += { "MemStatAuditor" }; // Set output level threshold (2=DEBUG,3=INFO,4=WARNING,5=ERROR,6=FATAL) MemStatAuditor.OutputLevel = 4; MessageSvc.OutputLevel = 2; ApplicationMgr.EvtMax = 10000; TriggerConfig.sequenceListFileLocation = "realseqlist.xml"; TriggerConfig.signatureListFileLocation = "realsiglist.xml"; //... Lvl1Conversion_L2.useL1Simulation = "NO"; Lvl1Conversion_L2.useMuons = "NO"; //... Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 13

14 Tests Ongoing tests of stability and consistence, bugs finding Performance tests Combinatoric explosure checks P4-2GHz standalone, simple menu and sequences: 6-10ms for 1 Event Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 14

15 Current status and outlook Steering, Navigation, Processing buffer, some real algorithms (electromagnetic, partially muon) Performance tests Completing the system Johannes Gutenberg Universität Mainz The ATLAS Trigger System, p. 15

4. LHC experiments Marcello Barisonzi LHC experiments August

4. LHC experiments Marcello Barisonzi LHC experiments August 4. LHC experiments 1 Summary from yesterday: Hadron colliders play an important role in particle physics discory but also precision measurements LHC will open up TeV energy range new particles with 3-5

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

2 ATLAS operations and data taking

2 ATLAS operations and data taking The ATLAS experiment: status report and recent results Ludovico Pontecorvo INFN - Roma and CERN on behalf of the ATLAS Collaboration 1 Introduction The ATLAS experiment was designed to explore a broad

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

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

ATLAS EXPERIMENT : HOW THE DATA FLOWS. (Trigger, Computing, and Data Analysis)

ATLAS EXPERIMENT : HOW THE DATA FLOWS. (Trigger, Computing, and Data Analysis) ATLAS EXPERIMENT : HOW THE DATA FLOWS (Trigger, Computing, and Data Analysis) In order to process large volumes of data within nanosecond timescales, the trigger system is designed to select interesting

More information

Dr. Andrea Bocci. Using GPUs to Accelerate Online Event Reconstruction. at the Large Hadron Collider. Applied Physicist

Dr. Andrea Bocci. Using GPUs to Accelerate Online Event Reconstruction. at the Large Hadron Collider. Applied Physicist Using GPUs to Accelerate Online Event Reconstruction at the Large Hadron Collider Dr. Andrea Bocci Applied Physicist On behalf of the CMS Collaboration Discover CERN Inside the Large Hadron Collider at

More information

ATLAS Level-1 trigger studies for the invisibly decaying Higgs boson produced in vector boson fusion

ATLAS Level-1 trigger studies for the invisibly decaying Higgs boson produced in vector boson fusion ATLAS Level-1 trigger studies for the invisibly decaying Higgs boson produced in vector boson fusion Guilherme Nunes Hanninger Markus Schumacher (Uni Siegen) Maria Laach, Sept. 2007 Invisibly decaying

More information

First Physics at LHC with ATLAS

First Physics at LHC with ATLAS First Physics at LHC with ATLAS Muon trigger efficiency The Large Hadron Collider Figure 1: The LHC accelerator chain[7]. The Large Hadron Collider (LHC), is a circular accelerator built at CERN. It is

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 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

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

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

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

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

Particle detection 1

Particle detection 1 Particle detection 1 Recall Particle detectors Detectors usually specialize in: Tracking: measuring positions / trajectories / momenta of charged particles, e.g.: Silicon detectors Drift chambers Calorimetry:

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

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

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

A glance at LHC Detector Systems. Burkhard Schmidt, CERN PH-DT

A glance at LHC Detector Systems. Burkhard Schmidt, CERN PH-DT A glance at LHC Detector Systems Burkhard Schmidt, CERN PH-DT The Enter LHC a New accelerator Era in Fundamental and the detectors Science Start-up of the Large Hadron Collider (LHC), one of the largest

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

Triggering at the Frontier: Top Quark Physics at ATLAS

Triggering at the Frontier: Top Quark Physics at ATLAS Triggering at the Frontier: Top Quark Physics at ATLAS Institutskolloquium Technisch Universität Dresden 23. April 2009 Martin zur Nedden, Humboldt-Universität zu Berlin 1 Content Open Questions The Large

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

Higgs cross-sections

Higgs cross-sections Ph.D. Detailed Research Project Search for a Standard Model Higgs boson in the H ZZ ( ) 4l decay channel at the ATLAS Experiment at Cern Ph.D. Candidate: Giacomo Artoni Supervisor: Prof. Carlo Dionisi,

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

Jet Calibration Issues in t t Events

Jet Calibration Issues in t t Events Jet Calibration Issues in t t Events Andreas Jantsch Max-Planck-Institut für Physik Munich 39. Herbstschule für Hochenergiephysik Maria Laach A. Jantsch (MPI für Physik) Jet Calibration Issues in t t Events

More information

Status and Performance of the ATLAS Experiment

Status and Performance of the ATLAS Experiment Status and Performance of the ATLAS Experiment P. Iengo To cite this version: P. Iengo. Status and Performance of the ATLAS Experiment. 15th International QCD Conference (QCD 10), Jun 2010, Montpellier,

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

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

ATLAS: Status and First Results

ATLAS: Status and First Results ATLAS: Status and First Results, University of Sheffield, on behalf of the ATLAS Collaboration 1 Overview of the ATLAS detector Status of the experiment Performance and physics results in the first six

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

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

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

The trigger system of the ATLAS experiment

The trigger system of the ATLAS experiment TU Dresden, IKTP Institutsseminar, 22.11.2007 The trigger system of the ATLAS experiment Johannes Haller (Universität Hamburg) Outline Important questions in particle physics The Large Hadron Collider

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

LHC State of the Art and News

LHC State of the Art and News LHC State of the Art and News ATL-GEN-SLIDE-2010-139 16 June 2010 Arno Straessner TU Dresden on behalf of the ATLAS Collaboration FSP 101 ATLAS Vulcano Workshop 2010 Frontier Objects in Astrophysics and

More information

CMS Status and the US-CMS DAQ projects

CMS Status and the US-CMS DAQ projects CMS Status and the US-CMS DAQ projects Ichiro Suzuki Fermi National Accelerator Laboratory KEK Seminar, 2003/03/24 1 Contents What am I talking about? Introduction What are we going to do? Physics topics

More information

(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.

(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system. Introduction One of the main events in the field of particle physics at the beginning of the next century will be the construction of the Large Hadron Collider (LHC). This machine will be installed into

More information

Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC

Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC WDS'12 Proceedings of Contributed Papers, Part III, 142 146, 212. ISBN 978-8-7378-226-9 MATFYZPRESS Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC I. Chalupková, Z.

More information

Physics at the LHC. Academic Training, Part 3: Experiment and Standard Model

Physics at the LHC. Academic Training, Part 3: Experiment and Standard Model Physics at the LHC Academic Training, Part 3: Experiment and Standard Model Dr. Sven Moch, DESY Zeuthen (Theory) Dr. (Experiment) June 2007 DESY Zeuthen, based on a lecture in WS 06/07 at Humboldt University

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

Trigger di primo livello per gli esperimenti ATLAS & CMS ad LHC

Trigger di primo livello per gli esperimenti ATLAS & CMS ad LHC Trigger di primo livello per gli esperimenti ATLAS & CMS ad LHC F.Pastore INFN Sezione di Roma II Workshop sulla fisica di ATLAS e CMS Napoli, 13-15 Ottobre 2004 Outline LHC Physics Program Requirements

More information

Z boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011

Z boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011 Z boson studies at the ATLAS experiment at CERN Giacomo Artoni Ph.D Thesis Project June 6, 2011 Outline Introduction to the LHC and ATLAS ((Very) Brief) Z boson history Measurement of σ Backgrounds Acceptances

More information

LHCb: From the detector to the first physics results

LHCb: From the detector to the first physics results LHCb: From the detector to the first physics results Olivier Callot Laboratoire de l Accélérateur Linéaire, IN2P3/CNRS and Université Paris XI, Orsay, France On behalf of the LHCb collaboration In this

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

Deep generative models for fast shower simulation in ATLAS

Deep generative models for fast shower simulation in ATLAS Deep generative models for fast shower simulation in ATLAS Dalila Salamani University of Geneva dalila.salamani@cern.ch On behalf of the ATLAS collaboration 14th e-science IEEE International Conference

More information

B-physics with ATLAS and CMS

B-physics with ATLAS and CMS Physics at LHC-2008 Split-CROATIA, 29.9. 4.10.2008 B-physics with ATLAS and CMS Brigitte Epp, Astro- and Particle Physics, University of Innsbruck, Austria representing ATLAS / CMS collaborations B-physics

More information

Discovery of the W and Z 0 Bosons

Discovery of the W and Z 0 Bosons Discovery of the W and Z 0 Bosons Status of the Standard Model ~1980 Planning the Search for W ± and Z 0 SppS, UA1 and UA2 The analyses and the observed events First measurements of W ± and Z 0 masses

More information

Early physics with the LHCb detector

Early physics with the LHCb detector XXVIII PHYSICS IN COLLISION - Perugia, Italy, June, 25-28, 2008 Early physics with the LHCb detector Dirk Wiedner CERN for the LHCb collaboration 27 June 2008 Dirk Wiedner at PIC2008 Perugia 1 Outline

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

Search for Displaced Supersymmetry using the Compact Muon Solenoid Detector

Search for Displaced Supersymmetry using the Compact Muon Solenoid Detector Search for Displaced Supersymmetry using the Compact Muon Solenoid Detector L. Antonelli, F. Blekman, A. Hart, N. Heracleous, C. Hill, B. Liu, and Q. Python for the CMS Collaboration 1 Outline Motivation!

More information

Hadronic Exotica Searches at CMS

Hadronic Exotica Searches at CMS Hadronic Exotica Searches at CMS Dinko Ferenček Rutgers, The State University of New Jersey On behalf of the CMS Collaboration SEARCH2012 Workshop March 19, 2012 College Park, Maryland Introduction and

More information

Introduction of CMS Detector. Ijaz Ahmed National Centre for Physics, Islamabad

Introduction of CMS Detector. Ijaz Ahmed National Centre for Physics, Islamabad Introduction of CMS Detector Ijaz Ahmed National Centre for Physics, Islamabad Layout of my Lectures: 1) Introduction of CMS Detector 2) CMS sub-detectors 3) CMS Trigger System Contents Introduction of

More information

AIM AIM. Study of Rare Interactions. Discovery of New High Mass Particles. Energy 500GeV High precision Lots of events (high luminosity) Requirements

AIM AIM. Study of Rare Interactions. Discovery of New High Mass Particles. Energy 500GeV High precision Lots of events (high luminosity) Requirements AIM AIM Discovery of New High Mass Particles Requirements Centre-of-Mass energy > 1000GeV High Coverage Study of Rare Interactions Requirements Energy 500GeV High precision Lots of events (high luminosity)

More information

The ATLAS Detector at the LHC

The ATLAS Detector at the LHC The ATLAS Detector at the LHC Results from the New Energy Frontier Cristina Oropeza Barrera Experimental Particle Physics University of Glasgow Somewhere near the Swiss Alps... A Toroidal LHC ApparatuS

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

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

Boosted searches for WW/WZ resonances in

Boosted searches for WW/WZ resonances in Boosted searches for WW/WZ resonances in the lνj final state BILLIE LUBIS COLUMBIA UNIVERSITY REU 2016 CERN Founded in 1954 by 12 Western European countries Now 22 member countries Aims to conduct cutting-edge

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

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

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

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

Jets triggers for the ATLAS experiment

Jets triggers for the ATLAS experiment Jets triggers for the ATLAS experiment Measurement of Global Trigger Efficiency for Multi-Jets analysis Luz Stella Gómez Fajardo Humboldt-Universität zu Berlin-GK DESY, Zeuthen Blockcourse, Rathen 08.04.2011

More information

Optimizing Selection and Sensitivity Results for VV->lvqq, 6.5 pb -1, 13 TeV Data

Optimizing Selection and Sensitivity Results for VV->lvqq, 6.5 pb -1, 13 TeV Data 1 Optimizing Selection and Sensitivity Results for VV->lvqq, 6.5 pb, 13 TeV Supervisor: Dr. Kalliopi Iordanidou 215 Columbia University REU Home Institution: High Point University 2 Summary Introduction

More information

An Introduction to my Recent Work. for the University of Oklahoma. Matthew Tamsett, RHUL

An Introduction to my Recent Work. for the University of Oklahoma. Matthew Tamsett, RHUL Matthew Tamsett An Introduction to my Recent Work for the University of Oklahoma 1 Overview This talk aims to: Give an overview of my experience as a physicist. Demonstrate my scientific and technical

More information

Higgs Boson Physics. Analysis Techniques. Günter Quast, Roger Wolf, Andrew Gilbert Master-Kurs SS

Higgs Boson Physics. Analysis Techniques. Günter Quast, Roger Wolf, Andrew Gilbert Master-Kurs SS Higgs Boson Physics Analysis Techniques Günter Quast, Roger Wolf, Andrew Gilbert Master-Kurs SS 2015 Institut für Experimentelle Kernphysik KIT Universität des Landes Baden-Württemberg und nationales Forschungszentrum

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 1996/005 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Performance of the Silicon Detectors for the

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

LHCb Overview. Barbara Storaci on behalf of the LHCb Collaboration

LHCb Overview. Barbara Storaci on behalf of the LHCb Collaboration LHCb Overview Barbara Storaci on behalf of the LHCb Collaboration CERN Council, December 14 th, 2012 Overview Introduction Collaboration Type of physics considered Detector Detector performances Selection

More information

Particle Detectors A brief introduction with emphasis on high energy physics applications

Particle Detectors A brief introduction with emphasis on high energy physics applications Particle Detectors A brief introduction with emphasis on high energy physics applications TRIUMF Summer Institute 2006 July 10-21 2006 Lecture I measurement of ionization and position Lecture II scintillation

More information

The Collider Detector at Fermilab. Amitabh Lath Rutgers University July 25, 2002

The Collider Detector at Fermilab. Amitabh Lath Rutgers University July 25, 2002 The Collider Detector at Fermilab Amitabh Lath Rutgers University July 25, 2002 What is Fermilab? A user facility with the Tevatron: 4 mile ring with superconducting magnets. Collides protons with antiprotons.

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 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

Trigger in ATLAS and CMS

Trigger in ATLAS and CMS Trigger in ATLAS and CMS Christos Leonidopoulos CERN-PH On behalf of the ATLAS and CMS collaborations LHC New Physics Signatures Workshop January 5-11, 2008, Ann Arbor What are we trying to do? Find the

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

Chapter 2 Experimental Apparatus

Chapter 2 Experimental Apparatus Chapter 2 Experimental Apparatus 2.1 The Large Hadron Collider 2.1.1 Design The Large Hadron Collider (LHC) [1] was constructed between 1998 2008 at CERN, the European Centre for Nuclear Research. It occupies

More information

Study of the performance of the Level-1 track trigger in the ee channel in ATLAS at high luminosity LHC

Study of the performance of the Level-1 track trigger in the ee channel in ATLAS at high luminosity LHC Teknisk- naturvetenskaplig fakultet UTH-enheten Besöksadress: Angströmlaboratoriet Lägerhyddsvägen 1 Hus 4, Plan 0 Postadress: Box 536 751 21 Uppsala Telefon: 018-471 30 03 Telefax: 018-471 30 00 Hemsida:

More information

Performance of the FastTracKer in ATLAS

Performance of the FastTracKer in ATLAS Performance of the FastTracKer in ATLAS Maddalena Giulini under supervision of Prof. A. Schöning and Dr. T. Klimkovich Physikalisches Institut, Universität Heidelberg DPG Spring Conference, Mainz March

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 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

Recent CMS results on heavy quarks and hadrons. Alice Bean Univ. of Kansas for the CMS Collaboration

Recent CMS results on heavy quarks and hadrons. Alice Bean Univ. of Kansas for the CMS Collaboration Recent CMS results on heavy quarks and hadrons Alice Bean Univ. of Kansas for the CMS Collaboration July 25, 2013 Outline CMS at the Large Hadron Collider Cross section measurements Search for state decaying

More information

Particles and Universe: Particle detectors

Particles and Universe: Particle detectors Particles and Universe: Particle detectors Maria Krawczyk, Aleksander Filip Żarnecki March 31, 2015 M.Krawczyk, A.F.Żarnecki Particles and Universe 5 March 31, 2015 1 / 46 Lecture 5 1 Introduction 2 Ionization

More information

Reconstruction and identification of hadronic tau-decays in ATLAS

Reconstruction and identification of hadronic tau-decays in ATLAS Reconstruction and identification of hadronic tau-decays in ALAS F. arrade o cite this version: F. arrade. Reconstruction and identification of hadronic tau-decays in ALAS. au06, 9th International Workshop

More information

Studies of the performance of the ATLAS detector using cosmic-ray muons

Studies of the performance of the ATLAS detector using cosmic-ray muons Eur. Phys. J. C (2011) 71: 1593 DOI 10.1140/epjc/s10052-011-1593-6 Special Article - Tools for Experiment and Theory Studies of the performance of the ATLAS detector using cosmic-ray muons The ATLAS Collaboration

More information

ATLAS NOTE. August 25, Electron Identification Studies for the Level 1 Trigger Upgrade. Abstract

ATLAS NOTE. August 25, Electron Identification Studies for the Level 1 Trigger Upgrade. Abstract Draft version 1.0 ATLAS NOTE August 25, 2012 1 Electron Identification Studies for the Level 1 Trigger Upgrade 2 3 4 L. Feremenga a, M.-A. Pleier b, F. Lanni b a University of Texas at Arlington b Brookhaven

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

Perspectives of Charmonium Production at CMS. Zongchang YANG, Peking University 1 st April, University of Virginia (USA)

Perspectives of Charmonium Production at CMS. Zongchang YANG, Peking University 1 st April, University of Virginia (USA) Perspectives of Charmonium Production at CMS Zongchang YANG, Peking University 1 st April, University of Virginia (USA) Outline Introduction to LHC, CMS and motivations Muon and di-muon trigger Muon and

More information

QCD cross section measurements with the OPAL and ATLAS detectors

QCD cross section measurements with the OPAL and ATLAS detectors QCD cross section measurements with the OPAL and ATLAS detectors Abstract of Ph.D. dissertation Attila Krasznahorkay Jr. Supervisors: Dr. Dezső Horváth, Dr. Thorsten Wengler University of Debrecen Faculty

More information

Status of the LHCb Experiment. Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001

Status of the LHCb Experiment. Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001 Status of the LHCb Experiment Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001 1 P b b P Number of pp inelastic interactions in one bunch crossing (σ inelastic = 80 mb): b b correlation

More information

Chapter 2 The CMS Experiment at the LHC

Chapter 2 The CMS Experiment at the LHC Chapter 2 The CMS Experiment at the LHC The Large Hadron Collider (LHC) [1] is designed to collide proton beams at a center-of-mass energy of s = 14 TeV and a nominal instantaneous luminosity of L = 10

More information

Experimental Methods of Particle Physics

Experimental Methods of Particle Physics Experimental Methods of Particle Physics (PHY461) Fall 015 Olaf Steinkamp 36-J- olafs@physik.uzh.ch 044 63 55763 Overview 1) Introduction / motivation measurement of particle momenta: magnetic field early

More information

Exotics Searches in Photon and Lepton Final States with the ATLAS Detector

Exotics Searches in Photon and Lepton Final States with the ATLAS Detector Exotics Searches in Photon and Lepton Final States with the ATLAS Detector Tetiana Berger-Hryn ova (LAPP, Annecy le Vieux) on behalf of the ATLAS collaboration EPS, Grenoble, France 21 July 2011 1 Introduction

More information

Search for a Lepton Flavor Violating Higgs Boson Using the Compact Muon Solenoid Detector at the Large Hadron Collider

Search for a Lepton Flavor Violating Higgs Boson Using the Compact Muon Solenoid Detector at the Large Hadron Collider Search for a Lepton Flavor Violating Higgs Boson Using the Compact Muon Solenoid Detector at the Large Hadron Collider University of Wisconsin-Madison 1 Outline Theoretical Background Standard Model Higgs

More information

LHC Detectors and their Physics Potential. Nick Ellis PH Department, CERN, Geneva

LHC Detectors and their Physics Potential. Nick Ellis PH Department, CERN, Geneva LHC Detectors and their Physics Potential Nick Ellis PH Department, CERN, Geneva 1 Part 1 Introduction to the LHC Detector Requirements & Design Concepts 2 What is the Large Hadron Collider? Circular proton-proton

More information

Self-organized mapping of calorimetry information for high efficient online electron/jet identification in ATLAS

Self-organized mapping of calorimetry information for high efficient online electron/jet identification in ATLAS Self-organized mapping of calorimetry information for high efficient online electron/jet identification in ATLAS Eduardo Simas Filho,, Luiz Caloba Signal Processing Laboratory, Federal University of Rio

More information

Electron Identification

Electron Identification Chapter 7 Electron Identification The identification of electrons is of fundamental importance to the ATLAS physics program. Leptons are the primary signature of electro-weak processes. They are used in

More information

PoS(ACAT)054. The Muon Trigger in ATLAS. Giovanni Siragusa d l,

PoS(ACAT)054. The Muon Trigger in ATLAS. Giovanni Siragusa d l, , Barria P. a i, Bellomo M. b j, Biglietti M. c k, Carlino G. c k, Cataldi G. l, Conventi F. c k, De Cecco S. a i, Di Mattia A. h, Dionisi C. a i, Falciano S. i, Giagu S. a i, Gorini E. d l, Grancagnolo

More information

Boosted decision tree performance studies in the t t τ + µ analysis at ATLAS

Boosted decision tree performance studies in the t t τ + µ analysis at ATLAS Boosted decision tree performance studies in the t t τ + µ analysis at ATLAS Allison MacDonald Supervised by Dr. Dugan O Neil Department of Physics, Simon Fraser University, Burnaby, British Columbia,

More information

Commissioning of the ATLAS LAr Calorimeter

Commissioning of the ATLAS LAr Calorimeter Commissioning of the ATLAS LAr Calorimeter S. Laplace (CNRS/LAPP) on behalf of the ATLAS Liquid Argon Calorimeter Group Outline: ATLAS in-situ commissioning steps Introduction to the ATLAS LAr Calorimeter

More information

La ricerca dell Higgs Standard Model a CDF

La ricerca dell Higgs Standard Model a CDF La ricerca dell Higgs Standard Model a CDF Melisa Rossi INFN-TS Giornata di seminari INFN Trieste - 7 Luglio 2009 FNAL: Fermi National Accelerator Lab Tevatron currently provides the highest energy proton-antiproton

More information

Reconstruction in Collider Experiments (Part IX)

Reconstruction in Collider Experiments (Part IX) Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part IX) Peter Loch University of Arizona Tucson,

More information