CMS Tracking Performance Results from early LHC Running
|
|
- Emmeline Reeves
- 8 years ago
- Views:
Transcription
1 CMS Tracking Performance Results from early LHC Running CMS PAPER TRK L. Spiegel, K. Stenson, M. Swartz 1
2 First Collisions Tracking Paper Provide description of tracker, tracking algorithm, and performance for summer conferences Based on already approved PAS TRK Add description of tracker (Sec 2) Modify description of triggers and data samples (Sec 3) Add description of pixel operating conditions, calibration, and performance (Sec 4.1) Add description of strip operating conditions, calibration, and performance (Sec 4.2) Expand PAS description of tracking algorithm (Sec 5) Condense description of tracking performance from PAS (Sec 6) Initiated/defined/reviewed by Tracker Editorial Board, Tracker DPG, Tracking/B-tag POG Conveners F. Palla, G. Hall, S. Nahn, D. Kotlinski, V. Chiochia, M. Manelli, J. Cole, G.M. Bilei, D. Contardo, C. Delaere, T. Speer, K. Burkett, A. Venturi, W. Adam, A. Rizzi Three editors L. Spiegel (new strip sections) K. Stenson (expanded tracking and condensed tracking performance) M. Swartz (new pixel sections) Same ARC as PAS: J. Alexander, V. Krutelyov, M. Pioppi Reports on the work of many collaborators from Tracker, Tracking/B-tag POGs 2
3 Preface Paper was written in February of 2010 All results based on December 2009 running at 900 GeV and 2360 GeV Results are non-uniform (understanding of pixel and strip systems were more/less advanced in many aspects) - subsystem results are not parallel Pixels and strips are different technologies with different readout schemes relevant parameters are different (eg. S/N meaningful for strips, not so much for pixels) non-parallel results Results that rely on detailed tracker simulation are not included eg. no tracking efficiency results, material studies, etc more and detailed papers in the near future Improved results based on 2010 data will be published in the coming year? 3
4 Pixel Detector Standard description of pixel system in Section 2 Subsection documents December operating conditions Bias voltages and temperature fraction of live channels = 98.4% Retuned readout thresholds lower than previously published CRAFT2008 effective in-time thresholds somewhat larger than test-pulse thresholds average layer efficiencies > 99% new analysis agrees with result reported in dn/dh paper Subsection documents the initial overall timing scan More recent fine scan results tested but still not in use Cluster size [pixel] CMS 1 Endcap Pixel Barrel Pixel Clock phase 3 [ns]
5 Pixel Section - Cluster Multiplicity Arbitrary scale TeV CMS data MC log (Number of Clusters) log (Number of Clusters) Compare measured cluster distribution at 900 GeV with Pythia/Geant ( Atlas tune) all triggers on left veto on BSC beam-gas trigger bits on right rough agreement is observed similar agreement with layer occupancies pixels working as expected in zeroth order discrepancies likely due to underlying event model 5
6 Pixel Section - Normalized Cluster Charge CMS 2009 s=900 GeV CMS 2009 s=900 GeV Number of clusters / 1[ke] MC DATA Barrel Number of clusters / 1[ke] MC DATA Endcap normalized cluster charge [ke] normalized cluster charge [ke] Scale cluster charge by track length to sensor thickness shows first results, work still in progress measured barrel width is larger than simulation charge smearing from incomplete gain corrections/imperfect calibration? ~5% scale shift in endcaps gain or threshold issues? electronic saturation not modeled correctly 6
7 Pixel Section Lorentz Angles Published CRAFT 2008 results are obsolete due to voltage and temperature changes. Note that the detailed Pixelav simulation is actually what is calibrated Correct Generic Reco/Simulation for implant focusing effects Generate Template profiles CRAFT2009 is only calibration for endcaps Deploy new grazing angle technique for barrel uses 2D segmentation of pixels Improved low PT tracking enables cluster size technique for barrel drift ["m] Offset ! tan( L ) 0.399! GeV data, B = 3.8T linear fit Grazing Angle Technique depth ["m] Sample Detector Technique Meas tanql Pixelav tanql CRAFT 2009 Barrel Cluster size 0.409± ±0.002 CRAFT 2009 Endcap Cluster size 0.081± ±0.004 Min Bias 2009 Barrel Grazing Angle 0.399± ±0.001 MIn Bias 2009 Barrel Cluster size 0.409± ±
8 Pixel Section Resolution Update CRAFT 2008 barrel module overlap analysis using Min Bias 2009 data. Coordinate Clusters Meas Resolution Pixelav Resolution local x (f) all 12.8±0.9mm local x (f) no double pixels 12.7±2.3mm 14.1±0.5mm local y (z) all 32.4±1.4mm local y (z) no double pixels 28.2±1.9mm 24.1±0.5mm Remove small charge clusters and edge clusters from the analysis Consider the effect of double-size pixels on the result double size pixels span Readout Chip boundaries including them worsens resolution wrt typical tracks (twice as probable in overlaps) Pixelav results don t include them Overlap x-resolutions are poorer than typical tracks populate the edges of the a-angle acceptance where resolution is poorer expect x-resolution < 10mm from Pixelav for most hits 8
9 Silicon Strip Detector Standard description of strip tracker in Section 2 Subsection 4.2 documents operating conditions Bias voltage, temperature of sensors and hybrids Distinction between peak and deconvolution operating modes of the APV25 A transition was made to deconvolution toward the end of the Early Collision period. Timing much more critical in deconvolution (hence the timing scan) Total integrated strip efficiency given at 97.8% Consistent with 2.2% bad modules and <0.2%(!) construction bad channel rate No detailed layer information. Documented in CRAFT Histogram and result collections Approved pixel, strip, and tracking results (includes 2360 GeV data as well) Staging area for plots to be approved for TRK No Lorentz angle results as they were not sufficiently mature at the time when the paper was written. 9
10 Strip Section S/N Plots shown for 2.36 TeV deconvolution mode illustrating the Landau nature of the signal and the difference between thin and thick sensors. The deco mode admits more noise than the peak mode, but there is no reason to expect changes in the S/N with changes in the center-of-mass energy. 10
11 Strip Section Timing Scan Most of the running was done in Peak mode Timing taken from CRAFT Reference to CMS note 2008/007 A fine scan was made close to the end of the collision period run , TOB layer 3 delays were implemented just before transition to Deconvolution mode (run ) No Peak data with fine scan delays 10 ns timing adjustment S/N reduced by 2.5% in Peak mode 11
12 Strip Section de/dx Strip tracker benefits from the large dynamic range in the APV25 analog based readout Up to 3 normal incidence MIPs in Early Collision running but will eventually be expanded to 7-8 MIPs Pixels are including in tracking but not in the de/dx determination Upper plot shows bands for kaons and protons and to a lesser extent deuterons. Fit is based on the proton band. Deuterons suffer from ADC saturation which is enhanced by the relatively larger η values. Pythia does not produce deuterons at all and there is some evidence that GEANT underproduces deuterons 12
13 Tracking results Section 5 gives a brief description of track reconstruction Section 6 gives tracking results. All of these results come from December 2009 data and were approved for the TRK PAS. Data/MC comparison of track variables (#tracks, hits/track, c 2, p T, h, f, d 0, d z ) Primary vertex resolution K S, L 0, X ±, K * (892) ± masses and resolution K S and L 0 lifetime de/dx tested on L 0 and used on f -> K + K Conversion mass, p T, and probability Nuclear interaction vertex position vs r and z b-tagging variables 3D IP significance and 3D vertex separation significance Plus the 4-track vertex event display (approved elsewhere) 13
14 Tracking distributions 14
15 Primary vertex resolution Split one primary vertex into two groups of tracks which must originate from the same point. Fit the two independent vertices and extract resolution. 15
16 V 0 mass distribution Data mass (MeV) MC mass (MeV) PDG mass (MeV) K S ± ± ± 0.02 L ± ± ± Data s (MeV) MC s (MeV) K S 7.99 ± ± 0.03 L ± ±
17 V 0 lifetimes Data and MC are split into bins of ct and a fit for the yield is performed in each bin. Divide MC yields by true (exponential) distribution to obtain correction factor. Correct data and fit for lifetime. For K S find 89.8 ± 2.1 ps compared to PDG of ± 0.05 ps For L 0 find 271 ± 20 ps compared to PDG of ± 2.0 ps. uncorrected data corrected data 17
18 X ± and K*(892) ± Take L 0 and try to vertex with a detached p to find a X. Take K S and combine with a primary p ± to find a K * (892) ±. 18
19 de/dx Left (right) plot is de/dx of low (high) momentum track in L 0 decay Hard track is always the proton follows proton curve f peak seen with de/dx cut on kaons; no f seen when fail de/dx cut 19
20 Conversions and interactions Photon conversion invariant mass, p T, and probability Radius and z positions of interaction vertices 20
21 b-tagging variables and 4-track detached vertex 21
22 Next Steps ARC Report (J. Alexander) and approval? Collaboration-Wide Review Please send comments to TRK hypernews Thanks to F. Palla/Tracker Editorial Board, Tracker DPG, Tracking/B-Tag POGs, ARC Big thanks to the many unnamed contributors to the paper! 22
Tracking/Vertexing/BeamSpot/b-tag Results from First Collisions (TRK-10-001)
Tracking/Vertexing/BeamSpot/b-tag Results from First Collisions (TRK-1-1) Yanyan Gao, Fermilab on behalf of Tracking-Btagging POGs 3 March 21 / CERN CMS General Weekly Meeting: GWM8 Contributors and Acknowledgement
More informationarxiv:1007.1988v2 [physics.ins-det] 27 Jul 2010 The CMS Collaboration
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH (CERN) CERN-PH-EP/-19 /7/14 -TRK--1 Tracking Performance Results from Early LHC Operation arxiv:7.1988v [physics.ins-det] 7 Jul The Collaboration Abstract The
More informationJet Reconstruction in CMS using Charged Tracks only
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
More informationThe accurate calibration of all detectors is crucial for the subsequent data
Chapter 4 Calibration The accurate calibration of all detectors is crucial for the subsequent data analysis. The stability of the gain and offset for energy and time calibration of all detectors involved
More informationProton tracking for medical imaging and dosimetry
Proton tracking for medical imaging and dosimetry J.Taylor, P.Allport, G.Casse For the PRaVDA Consortium 1 Background and motivation - What is the PRaVDA experiment? - Why are we using Monte Carlo? GEANT4
More informationPrecision Tracking Test Beams at the DESY-II Synchrotron. Simon Spannagel DPG 2014 T88.7 Mainz, 26.3.2014
Precision Tracking Test Beams at the DESY-II Synchrotron. Simon Spannagel DPG 2014 T88.7 Mainz, 26.3.2014 Overview > Test Beams at DESY-II > Tracking with the DATURA Telescope Telescope Hardware Software
More informationCalorimetry in particle physics experiments
Calorimetry in particle physics experiments Unit n. 8 Calibration techniques Roberta Arcidiacono Lecture overview Introduction Hardware Calibration Test Beam Calibration In-situ Calibration (EM calorimeters)
More informationTrack Trigger and Modules For the HLT
CMS L1 Track Trigger for SLHC Anders Ryd for the CMS Track Trigger Task Force Vertex 2009 Sept. 13-18, 2009 L=1035 cm-2s-1 Outline: SLHC trigger challenge Tracking triggers Track trigger modules Simulation
More informationCMS Physics Analysis Summary
Available on the CERN CDS information server CMS PAS RK-10-002 CMS Physics Analysis Summary Contact: cms-pog-conveners-tracking@cern.ch 2010/07/20 Measurement of racking Efficiency he CMS Collaboration
More informationElectron-Muon Ranger (EMR)
Electron-Muon Ranger (EMR) Digitization and Reconstruction François Drielsma Ruslan Asfandiyarov University of Geneva On Behalf of the EMR Group 38 th MICE Collaboration Meeting February 23, 2014 Electron-Muon
More informationSilicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection -
timo.peltola@helsinki.fi Finnish Society for Natural Philosophy, Helsinki, 17 February 2015 Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection - Timo Peltola
More informationReal Time Tracking with ATLAS Silicon Detectors and its Applications to Beauty Hadron Physics
Real Time Tracking with ATLAS Silicon Detectors and its Applications to Beauty Hadron Physics Carlo Schiavi Dottorato in Fisica - XVII Ciclo Outline The ATLAS Experiment The SiTrack Algorithm Application
More informationOperation and Performance of the CMS Silicon Tracker
Operation and Performance of the CMS Silicon Tracker Manfred Krammer 1 on behalf of the CMS Tracker Collaboration Institute of High Energy Physics, Austrian Academy of Sciences, Vienna, Austria Abstract.
More informationOffline Tracker DQM Shi1 Tutorial
Offline Tracker DQM Shi1 Tutorial Tracker Shi1s Overview Online Shi1s at P5 (3/day for 24 hours coverage) One Pixel shi1er and one SiStrip shi1er for 8h shi1s One Pixel shi1 leader and one SiStrip shi1
More informationarxiv:1402.0675v1 [physics.ins-det] 4 Feb 2014
Preprint typeset in JINST style - HYPER VERSION Operation and performance of the CMS tracker arxiv:1402.0675v1 [physics.ins-det] 4 Feb 2014 Viktor Veszpremi for the CMS Collaboration a a Wigner Research
More informationLarge Hadron Collider am CERN
The CMS Silicon Tracker Lutz Feld 1. Physikalisches Institut, RWTH Aachen GSI Darmstadt, 18. 4. 2007 Large Hadron Collider am CERN proton proton quarks & gluons circumference 27 km 1200 superconducting
More informationVertex and track reconstruction with the ALICE Inner Tracking System
Vertex and track reconstruction with the ALICE Inner Tracking System The 5th International Nordic "LHC and Beyond" Workshop St.Petersburg, 8-11 June 2010 Leonardo Milano Univ. & INFN, Torino for the ALICE
More informationThe LHCb Tracking System. Jeroen van Hunen
The LHCb Tracking System Jeroen van Hunen The LHCb Experiment LHCb at Point 8 : a lot of activity! LHCb : a B-physics experiment that is being constructed for : Precision measurements of the CPviolation
More informationA.Besson, IPHC-Strasbourg
DIGMAPS: a standalone tool to study digitization an overview of a digitizer strategy for CMOS/MAPS sensors A.Besson, IPHC-Strasbourg thanks to A.Geromitsos and J.Baudot Motivations for a CMOS sensor digitizer,
More informationInformation about the T9 beam line and experimental facilities
Information about the T9 beam line and experimental facilities The incoming proton beam from the PS accelerator impinges on the North target and thus produces the particles for the T9 beam line. The collisions
More informationDetector-related. related software development in the HEPP project. Are Strandlie Gjøvik University College and University of Oslo
Detector-related related software development in the HEPP project Are Strandlie Gjøvik University College and University of Oslo Outline Introduction The ATLAS New Tracking project HEPP contributions Summary
More informationCharacterisation of the Timepix Chip for the LHCb VELO Upgrade
Particle and Astroparticle Physics Master Thesis Characterisation of the Timepix Chip for the LHCb VELO Upgrade Veerle Heijne Supervisor: Dr. Martin van Beuzekom Second reviewer: Dr. Auke-Pieter Colijn
More informationPoS(Kruger 2010)013. Setting of the ATLAS Jet Energy Scale. Michele Petteni Simon Fraser University E-mail: mpetteni@sfu.ca
Setting of the ALAS Energy Scale Simon Fraser University E-mail: mpetteni@sfu.ca he setting of the energy scale and its uncertainty in the ALAS detector is presented. After a brief introduction of the
More informationAC coupled pitch adapters for silicon strip detectors
AC coupled pitch adapters for silicon strip detectors J. Härkönen1), E. Tuovinen1), P. Luukka1), T. Mäenpää1), E. Tuovinen1), E. Tuominen1), Y. Gotra2), L. Spiegel2) Helsinki Institute of Physics, Finland
More informationValidation of the MadAnalysis 5 implementation of ATLAS-SUSY-13-05
Validation of the MadAnalysis 5 implementation of ATLAS-SUSY-3-5 Guillaume Chalons (LPSC Grenoble) email: chalons@lpsc.in2p3.fr October 27, 24 Abstract In this note we summarise our validation of the ATLAS
More informationFTK the online Fast Tracker for the ATLAS upgrade
FTK the online Fast Tracker for the ATLAS upgrade Kostas Kordas Aristotle University of Thessaloniki Annual EESFYE mtg, University of the Aegean, Chios, 25-29 April 2013 Overview ATLAS Trigger and DAQ
More informationTop rediscovery at ATLAS and CMS
Top rediscovery at ATLAS and CMS on behalf of ATLAS and CMS collaborations CNRS/IN2P3 & UJF/ENSPG, LPSC, Grenoble, France E-mail: julien.donini@lpsc.in2p3.fr We describe the plans and strategies of the
More informationPerformance Evalua/on and So2ware Development of FPCCD Vertex Detector for ILC
Performance Evalua/on and So2ware Development of FPCCD Vertex Detector for ILC MORI Tatsuya, KAMAI Daisuke, MIYAMOTO Akiya A SUGIMOTO Yasuhiro A, ISHIKAWA Akimasa, SUEHARA Taikan, KATO Eriko, YAMAMOTO
More informationvariables to investigate Monte Carlo methods of t t production
Using the M 2 and variables to investigate Monte Carlo methods of t t production Caitlin Jones September 8, 25 Abstract In this project the behaviour of Monte Carlo simulations for the event t t! ` `+b
More informationRadiation Hard Sensor Materials for the CMS Tracker Upgrade The CMS HPK Campaign
Radiation Hard Sensor Materials for the CMS Tracker Upgrade The CMS HPK Campaign on behalf of the CMS Tracker Collaboration Institut für Experimentelle Kernphysik, KIT Germany KIT University of the State
More informationCMS Level 1 Track Trigger
Institut für Technik der Informationsverarbeitung CMS Level 1 Track Trigger An FPGA Approach Management Prof. Dr.-Ing. Dr. h.c. J. Becker Prof. Dr.-Ing. Eric Sax Prof. Dr. rer. nat. W. Stork KIT University
More informationThe TOTEM experiment at the LHC: results and perspective
The TOTEM experiment at the LHC: results and perspective Edoardo Bossini Università degli studi di Siena and INFN-Pisa (on behalf of the TOTEM collaboration) Trieste, 24 Settembre 2013 OUTLINE: Detector
More informationSilicon Seminar. Optolinks and Off Detector Electronics in ATLAS Pixel Detector
Silicon Seminar Optolinks and Off Detector Electronics in ATLAS Pixel Detector Overview Requirements The architecture of the optical links for the ATLAS pixel detector ROD BOC Optoboard Requirements of
More information(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier
(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier (no PiN and pinned Diodes) Peter Fischer P. Fischer, ziti, Uni Heidelberg, Seite 1 Overview Reminder: Classical Photomultiplier
More informationHall B So(ware Status. Veronique Ziegler
Hall B So(ware Status Veronique Ziegler Physics Applica;on Design within the ClaRA SOA Physics applica;on design/composi;on based on services Development of services within ClaRA à Wri;ng a service simply
More informationElectronics GRETINA Project
Electronics GRETINA Project Requirement Document Sergio Zimmermann July 24, 2004 ANL Electronics Workshop, Schedule 1 Outline Doc Data Base Justification Document types Functional requirements List of
More informationPerformance of the CMS cathode strip chambers with cosmic rays
Home Search Collections Journals About Contact us My IOPscience Performance of the CMS cathode strip chambers with cosmic rays This article has been downloaded from IOPscience. Please scroll down to see
More informationLarge Hadron Collider LHC will explore a new energy domain: the Terascale
The CMS All Silicon Tracker A Detector for the Exploration of the Terascale Lutz Feld 1. Physikalisches Institut, RWTH Aachen Heidelberg, 23. 3. 2007 The LHC Physics Program Large Hadron Collider LHC will
More informationEvaluation Tools for the Performance of a NESTOR Test Detector
Evaluation Tools for the Performance of a NESTOR Test Detector G. Bourlis, A. Leisos, S. E. Tzamarias and A. Tsirigotis Particle and Astroparticle Physics Group School of Science and Technology Hellenic
More informationMICE detectors and first results. M. Bonesini Sezione INFN Milano Bicocca
MICE detectors and first results M. Bonesini Sezione INFN Milano Bicocca I will speak of the installed beamline PID detectors (TOFes, CKOVs, KL) and only shortly of EMR (to be built)/ the trackers (tested
More informationThe CMS All Silicon Tracker
The CMS All Silicon Tracker A Detector for the Exploration of the Terascale Lutz Feld 1. Physikalisches Institut, RWTH Aachen Göttingen, 25. 1. 2008 Large Hadron Collider at CERN proton proton quarks &
More informationRecent SiD Tracking Studies at CU (and Ancient Outer Tracker Studies at SLAC)
Recent SiD Tracking Studies at CU (and Ancient Outer Tracker Studies at SLAC) Steve Wagner, University of Colorado, Boulder I did realistic pattern recognition studies for the SiD Barrel Outer Tracker
More informationMATRIX TECHNICAL NOTES
200 WOOD AVENUE, MIDDLESEX, NJ 08846 PHONE (732) 469-9510 FAX (732) 469-0418 MATRIX TECHNICAL NOTES MTN-107 TEST SETUP FOR THE MEASUREMENT OF X-MOD, CTB, AND CSO USING A MEAN SQUARE CIRCUIT AS A DETECTOR
More informationComparisons between 2003 CMS ECAL TB data and a Geant 4 MC
Comparisons between 2003 CMS CAL TB data and a Geant 4 MC P. Meridiani LCG Validation Meeting 7 th July 2004 Outline CMS lectromagnetic calorimeter and 2003 TB h4sim http://cmsdoc.cern.ch/~h4sim/ (What
More informationPart 4 fitting with energy loss and multiple scattering non gaussian uncertainties outliers
Part 4 fitting with energy loss and multiple scattering non gaussian uncertainties outliers material intersections to treat material effects in track fit, locate material 'intersections' along particle
More informationThe OPERA Emulsions. Jan Lenkeit. Hamburg Student Seminar, 12 June 2008. Institut für Experimentalphysik Forschungsgruppe Neutrinophysik
The OPERA Emulsions Jan Lenkeit Institut für Experimentalphysik Forschungsgruppe Neutrinophysik Hamburg Student Seminar, 12 June 2008 1/43 Outline The OPERA experiment Nuclear emulsions The OPERA emulsions
More informationElectron-Muon Ranger (EMR)
Electron-Muon Ranger (EMR) Ruslan Asfandiyarov MICE Video Conference April 11, 2013 Construction Construction quarter of the detector completed (12 planes) every plane tested (LED / Camera / image analysis)
More informationElectron Muon Ranger (EMR) Software Development
Electron Muon Ranger (EMR) Software Development François Drielsma on behalf of the EMR Group University of Geneva June 25, 2014 François Drielsma on behalf of the EMR Group Electron (University Muon of
More informationMars Atmosphere and Volatile EvolutioN (MAVEN) Mission
Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission MAVEN Science Community Workshop December 2, 2012 Particles and Fields Package Solar Energetic Particle Instrument (SEP) Davin Larson and the SEP
More informationSilicon Lab Bonn. Physikalisches Institut Universität Bonn. DEPFET Test System Test Beam @ DESY
Silicon Lab Bonn Physikalisches Institut Universität Bonn DEPFET Test System Test Beam @ DESY H. Krüger, EUDET Brainstorming, 3/4.11.2005 1 SI LAB DEPFET Prototype System DEPFET sensors 64 x 128 pixels,
More informationMPC 4. Machinery Protection Card Type MPC 4 FEATURES. Continuous on-line Machinery Protection Card
Machinery Protection Card Type FEATURES Continuous on-line Machinery Protection Card Real-time measurement and monitoring using state-of-the-art DSP techniques Fully VME-compatible slave interface Fully
More informationDevelopment of the electromagnetic calorimeter waveform digitizers for the Fermilab Muon g-2 experiment
Development of the electromagnetic calorimeter waveform digitizers for the Fermilab g-2 experiment 1 on behalf of the Fermilab E989 g-2 Collaboration European Physical Society Conference on High Energy
More informationCMS Tracker module / hybrid tests and DAQ development for the HL-LHC
CMS Tracker module / hybrid tests and DAQ development for the HL-LHC S. Mersi, G. Auzinger georg.auzinger@cern.ch 1 Outline Reminder: the Ph2 CMS Tracker upgrade pt Modules: principle, elements, electronics
More informationS2000 Spectrometer Data Sheet
Description The Ocean Optics OEM S2000 Spectrometer includes the linear CCD-array optical bench, plus the circuits necessary for spectrometer operation. The result is a compact, flexible system with no
More informationJets energy calibration in ATLAS
Jets energy calibration in ATLAS V.Giangiobbe Università di Pisa INFN sezione di Pisa Supported by the ARTEMIS Research Training Network Workshop sui Monte Carlo, la Fisica e le Simulazioni a LHC V.Giangiobbe
More informationRunning in 2011 - Luminosity. Mike Lamont Verena Kain
Running in 2011 - Luminosity Mike Lamont Verena Kain Presentations Many thanks to all the speakers! Experiments expectations Massi Ferro-Luzzi Pushing the limits: beam Elias Métral Pushing the limits:
More informationOther GEANT4 capabilities
Other GEANT4 capabilities Event biasing Parameterisation (fast simulation) Persistency Parallelisation and integration in a distributed computing environment Outline! Event biasing! Parameterization (fast
More informationMonte Carlo Simulations in Proton Dosimetry with Geant4
Monte Carlo Simulations in Proton Dosimetry with Geant4 Zdenek Moravek, Ludwig Bogner Klinik und Poliklinik für Strahlentherapie Universität Regensburg Objectives of the Study what particles and how much
More informationX- and Gamma Ray Imaging Systems based on CdTe-CMOS Detector Technology
X- and Gamma Ray Imaging Systems based on dte-mos Detector Technology Konstantinos Spartiotis, Ray Durrant, nssi Leppänen, Henrik Lohman, Olli Männistö, Tuomas Pantsar, Jouni Pyyhtiä, Tom Schulman, Oy
More informationSolid State Detectors = Semi-Conductor based Detectors
Solid State Detectors = Semi-Conductor based Detectors Materials and their properties Energy bands and electronic structure Charge transport and conductivity Boundaries: the p-n junction Charge collection
More informationChapter 8. Low energy ion scattering study of Fe 4 N on Cu(100)
Low energy ion scattering study of 4 on Cu(1) Chapter 8. Low energy ion scattering study of 4 on Cu(1) 8.1. Introduction For a better understanding of the reconstructed 4 surfaces one would like to know
More informationCalibration and performance test of the Very Front End electronics for the CMS electromagnetic calorimeter
Calibration and performance test of the Very Front End electronics for the CMS electromagnetic calorimeter Jan Blaha IPN Lyon 10th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD06)
More informationPerformance of Silicon N-in-P Pixel Detectors Irradiated up to 5 1015 neq /cm2 for Future ATLAS Upgrades
Performance of Silicon N-in-P Pixel Detectors Irradiated up to 5 1 neq /cm for Future ATLAS Upgrades Philipp Weigell1 Ch. A. La Rosa3, A. Macchiolo1, R. Nisius1, H. Pernegger3, R.H. Richter Gallrapp3,
More informationThe STAR Level-3 Trigger System
Jens Sören Lange University of Frankfurt The STAR Level-3 Trigger System C. Adler a, J. Berger a, M. DeMello b, D. Flierl a, J. Landgraf c, J.S. Lange a, M.J. LeVine c, A. Ljubicic Jr. c, J. Nelson d,
More informationPersonal Identity Verification (PIV) IMAGE QUALITY SPECIFICATIONS FOR SINGLE FINGER CAPTURE DEVICES
Personal Identity Verification (PIV) IMAGE QUALITY SPECIFICATIONS FOR SINGLE FINGER CAPTURE DEVICES 1.0 SCOPE AND PURPOSE These specifications apply to fingerprint capture devices which scan and capture
More informationSpike-Based Sensing and Processing: What are spikes good for? John G. Harris Electrical and Computer Engineering Dept
Spike-Based Sensing and Processing: What are spikes good for? John G. Harris Electrical and Computer Engineering Dept ONR NEURO-SILICON WORKSHOP, AUG 1-2, 2006 Take Home Messages Introduce integrate-and-fire
More informationCELL CYCLE BASICS. G0/1 = 1X S Phase G2/M = 2X DYE FLUORESCENCE
CELL CYCLE BASICS Analysis of a population of cells replication state can be achieved by fluorescence labeling of the nuclei of cells in suspension and then analyzing the fluorescence properties of each
More informationResults from first tests of TRD prototypes for CBM. DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main
Results from first tests of TRD prototypes for CBM DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Contents Overview of the CBM experiment CBM-TRD General TRD requirements The
More informationA Guide to Detectors Particle Physics Masterclass. M. van Dijk
A Guide to Particle Physics Masterclass M. van Dijk 16/04/2013 How detectors work Scintillation Ionization Particle identification Tracking Calorimetry Data Analysis W & Z bosons 2 Reconstructing collisions
More informationT(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades
T(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades R. Milinčić1, P. Gorham1, C. Hebert1, S. Matsuno1, P. Miočinović1, M. Rosen1, D. Saltzberg2, G. Varner1 1 University
More informationAN1200.04. Application Note: FCC Regulations for ISM Band Devices: 902-928 MHz. FCC Regulations for ISM Band Devices: 902-928 MHz
AN1200.04 Application Note: FCC Regulations for ISM Band Devices: Copyright Semtech 2006 1 of 15 www.semtech.com 1 Table of Contents 1 Table of Contents...2 1.1 Index of Figures...2 1.2 Index of Tables...2
More informationTHE CMS PIXEL DETECTOR: FROM PRODUCTION TO COMMISSIONING
THE CMS PIXEL DETECTOR: FROM PRODUCTION TO COMMISSIONING VINCENZO CHIOCHIA On behalf of the CMS Collaboration University of Zürich, Physik-Institut, Winterthurerstr. 190 Zürich, CH-8057, Switzerland The
More informationPoS(LHCPP2013)033. Rare B meson decays at LHC. Francesco Dettori Nikhef and Vrij Universiteit, Amsterdam E-mail: fdettori@nikhef.nl.
Nikhef and Vrij Universiteit, Amsterdam E-mail: fdettori@nikhef.nl Paolo Iengo INFN Napoli E-mail: paolo.iengo@cern.ch Luca Martini INFN Pisa E-mail: Luca.Martini@cern.ch Rare decays of B mesons are fundamental
More informationCalibrations, alignment, online data monitoring
DAQ & Software Review : Calibrations, alignment, online data monitoring Jlab June 18, 2014. Software Organization Software Analysis Chairs: Maurik Holtrop Mathew Graham Subsystem Leads: ECAL Stuart Fegan
More informationQualification of the CMS Barrel Pixel Detector Modules
Preprint typeset in JINST style - HYPER VERSION Qualification of the CMS Barrel Pixel Detector Modules Sarah Dambach 1,2, Christina Eggel 1,2, Urs Langenegger 1, Andrey Starodumov 2 and Peter Trüb 1,2
More informationATLAS NOTE ATLAS-CONF-2010-063. July 21, 2010. Search for top pair candidate events in ATLAS at s = 7 TeV. The ATLAS Collaboration.
ATLAS NOTE ATLAS-CONF-2010-063 July 21, 2010 Search for top pair candidate events in ATLAS at s = 7 TeV The ATLAS Collaboration Abstract A search is performed for events consistent with top quark pair
More informationStatus of ALICE activities within FKPPL LIA
Status of ALICE activities within FKPPL LIA 1 Development of the online monitoring software for the ALICE Muon Trigger And Suppression Study for Υ S A N G - U N A H N K O N K U K U N I V E R S I T Y S
More informationCross section, Flux, Luminosity, Scattering Rates
Cross section, Flux, Luminosity, Scattering Rates Table of Contents Paul Avery (Andrey Korytov) Sep. 9, 013 1 Introduction... 1 Cross section, flux and scattering... 1 3 Scattering length λ and λ ρ...
More informationMeasurement of the Mass of the Top Quark in the l+ Jets Channel Using the Matrix Element Method
Measurement of the Mass of the Top Quark in the l+ Jets Channel Using the Matrix Element Method Carlos Garcia University of Rochester For the DØ Collaboration APS Meeting 2007 Outline Introduction Top
More informationATLAS Test Beam Analysis in Stockholm: An Overview
ATLAS Test Beam Analysis in Stockholm: An Overview Elin Bergeås, Stockholm University Stand-alone test beam 2003 and before - test beam targeted at TileCal modules only Combined test beam 2004 - test beam
More informationPhysics 111 Homework Solutions Week #9 - Tuesday
Physics 111 Homework Solutions Week #9 - Tuesday Friday, February 25, 2011 Chapter 22 Questions - None Multiple-Choice 223 A 224 C 225 B 226 B 227 B 229 D Problems 227 In this double slit experiment we
More informationAN INVESTIGATION INTO THE USEFULNESS OF THE ISOCS MATHEMATICAL EFFICIENCY CALIBRATION FOR LARGE RECTANGULAR 3 x5 x16 NAI DETECTORS
AN INVESTIGATION INTO THE USEFULNESS OF THE ISOCS MATHEMATICAL EFFICIENCY CALIBRATION FOR LARGE RECTANGULAR 3 x5 x16 NAI DETECTORS Frazier L. Bronson CHP Canberra Industries, Inc. 800 Research Parkway,
More informationPhysik des Higgs Bosons. Higgs decays V( ) Re( ) Im( ) Figures and calculations from A. Djouadi, Phys.Rept. 457 (2008) 1-216
: Higgs decays V( ) Re( ) Im( ) Figures and calculations from A. Djouadi, Phys.Rept. 457 (2008) 1-216 1 Reminder 10.6.2014 Higgs couplings: 2 Reminder 10.6.2014 Higgs BF as a function of mh Higgs total
More informationDDX 7000 & 8003. Digital Partial Discharge Detectors FEATURES APPLICATIONS
DDX 7000 & 8003 Digital Partial Discharge Detectors The HAEFELY HIPOTRONICS DDX Digital Partial Discharge Detector offers the high accuracy and flexibility of digital technology, plus the real-time display
More informationOptical Link ASICs for LHC Upgrades
Optical Link ASICs for LHC Upgrades K.K. Gan, H.P. Kagan, R.D. Kass, J. Moore, S. Smith The Ohio State University July 30, 2009 K.K. Gan DPF2009 1 Outline Introduction VCSEL driver chip PIN receiver/decoder
More informationGamma-ray Large Area Space Telescope (GLAST) Large Area Telescope (LAT) Calorimeter AFEE Board Parts Radiation Test Plan
GLAST LAT DESIGN DESCRIPTION Document Title AFEE Board Parts Radiation Test Plan Document # Date Effective LAT-SS-01890-01 1 April 2003 Prepared by(s) Supersedes James Ampe None Subsystem/Office Calorimeter
More informationATLAS Tile Calorimeter Readout Electronics Upgrade Program for the High Luminosity LHC
ATLAS Tile Calorimeter Readout Electronics Upgrade Program for the High Luminosity LHC Augusto Santiago Cerqueira On behalf of the ATLAS Tile Calorimeter Group Federal University of Juiz de Fora, Brazil
More informationIEC 1000-4-2 ESD Immunity and Transient Current Capability for the SP72X Series Protection Arrays
IEC 00-4-2 ESD Immunity and Transient Current Capability for the SP72X Series Protection Arrays Application Note July 1999 AN9612.2 Author: Wayne Austin The SP720, SP721, SP723, and SP724 are protection
More informationTruly digital PET imaging
Advanced Molecular Imaging Vereos PET/CT Truly digital PET imaging Philips proprietary Digital Photon Counting technology Vereos PET/CT is the first commercially available scanner to offer truly digital
More informationSimulation of Neutron Backgrounds from the ILC Extraction Line Beam Dump. Siva Darbha. Office of Science, SULI Program. University of Toronto
SLAC-TN-07-013 August 2007 Simulation of Neutron Backgrounds from the ILC Extraction Line Beam Dump Siva Darbha Office of Science, SULI Program University of Toronto Stanford Linear Accelerator Center
More informationGRETA. I-Yang Lee. For the GRETA Steering Committee. Workshop on the Experimental Equipment for RIA March 18-22, 2003, Oak Ridge, Tennessee
GRETA I-Yang Lee For the GRETA Steering Committee Workshop on the Experimental Equipment for RIA March 18-22, 2003, Oak Ridge, Tennessee Gamma-ray Tracking Concepts Compton Suppressed Ge Veto Ν det = 100
More informationTop-Quark Studies at CMS
Top-Quark Studies at CMS Tim Christiansen (CERN) on behalf of the CMS Collaboration ICHEP 2010, Paris 35th International Conference on High-Energy Physics tt 2 km 22 28 July 2010 Single-top 4 km New Physics
More informationπ 0 γγ calibration Savrina Daria, ITEP, Moscow SINP MSU, Moscow Victor Egorychev, ITEP, Moscow Ivan Belyaev
π 0 γγ calibration Savrina Daria, ITEP, Moscow SINP MSU, Moscow Ivan Belyaev Victor Egorychev, ITEP, Moscow Loose cuts for π 0 selection One of the ways to improve the calibration procedure is to increase
More informationCLAS12 Offline Software Tools. G.Gavalian (Jlab)
CLAS12 Offline Software Tools G.Gavalian (Jlab) Overview Data formats I/O gemc data reader raw data reader detector hit decoder ET ring data reader Geometry Package implementation of all baseline detectors
More information07 - Cherenkov and transition radiation detectors
07 - Cherenkov and transition radiation detectors Jaroslav Adam Czech Technical University in Prague Version 1.0 Jaroslav Adam (CTU, Prague) DPD_07, Cherenkov and transition radiation Version 1.0 1 / 30
More informationHow To Teach Physics At The Lhc
LHC discoveries and Particle Physics Concepts for Education Farid Ould- Saada, University of Oslo On behalf of IPPOG EPS- HEP, Vienna, 25.07.2015 A successful program LHC data are successfully deployed
More informationEnergy Deposition in MICE Absorbers and Coils
in MICE Absorbers and Coils November 2, 2003 Video Conference Page 1 An Application for G4Mice We would like to estimate how much energy is deposited in magnet coils and the hydrogen absorber. Most of
More informationHigh Energy Physics. Lecture 4 More kinematics and a picture show of particle collisions
High Energy Physics Lecture 4 More kinematics and a picture show of particle collisions 1 Recall from the previous lecture: the momentum of the scattered Particle in an elastic collision is given by p
More informationClustering & Visualization
Chapter 5 Clustering & Visualization Clustering in high-dimensional databases is an important problem and there are a number of different clustering paradigms which are applicable to high-dimensional data.
More informationGE Medical Systems Training in Partnership. Module 8: IQ: Acquisition Time
Module 8: IQ: Acquisition Time IQ : Acquisition Time Objectives...Describe types of data acquisition modes....compute acquisition times for 2D and 3D scans. 2D Acquisitions The 2D mode acquires and reconstructs
More information