Jerry Blazey May 31, 2007 LCWS07 1 SiD Overview & Opportunities Jerry Blazey Northern Illinois University LCWS07-Hamburg.

Slides:



Advertisements
Similar presentations
TIME 2005: TPC for the ILC 6 th Oct 2005 Matthias Enno Janssen, DESY 1 A Time Projection Chamber for the International Linear Collider R&D Studies Matthias.
Advertisements

1 Individual Particle Reconstruction CHEP07, Victoria, September 6, 2007 Norman Graf (SLAC) Steve Magill (ANL)
The CMS Detector Paoti Chang National Taiwan University
Simulation Studies of a (DEPFET) Vertex Detector for SuperBelle Ariane Frey, Max-Planck-Institut für Physik München Contents: Software framework Simulation.
ILC detectors: 1)the SiD concept 2)detector R&D in the US Harry Weerts Argonne National Laboratory.
Testbeam Requirements for LC Calorimetry S. R. Magill for the Calorimetry Working Group Physics/Detector Goals for LC Calorimetry E-flow implications for.
H. Weerts SLAC SLUO meeting; Sept 18, 2008 SiD-- a compact detector for ILC H.Weerts for SiD detector concept Argonne National Lab.
7 Sept 2007Paul Dauncey - Calorimetry1 UK Opportunities in SiD Calorimetry Paul Dauncey Imperial College London.
7 June 2006 SLAC DOE Review M. Breidenbach 1 KPiX & EMCal SLAC –D. Freytag –G. Haller –R. Herbst –T. Nelson –mb Oregon –J. Brau –R. Frey –D. Strom BNL.
SLAC EPAC M. Breidenbach124 January 2006 SiD SLAC EPAC
The SiD concept Yannis Karyotakis LAPP Annecy / IN2P3 March 21 st ‘05.
“GLD” Detector Concept Study 21. Mar. Y. Sugimoto KEK.
1 Benchmarking the SiD Tim Barklow SLAC Sep 27, 2005.
SLUO M. Breidenbach126 September 2005 SiD SLUO
Snowmass, August 16, 2005 H.Weerts SiD Design Goals and Plans for Snowmass Snowmass H.Weerts Argonne Nat. Lab./ Michigan State Univ.
The GLD Concept. MDI Issues Impact on Detector Design L*  Background (back-scattered e+-, , n) into VTX, TPC Crossing angle  Minimum veto angle for.
David Attié Club ‘ILC Physics Case’ CEA Saclay June 23, 2013 ILD & SiD concepts and R&D.
Development of Particle Flow Calorimetry José Repond Argonne National Laboratory DPF meeting, Providence, RI August 8 – 13, 2011.
@ The SiD detector concept : An Introduction Harry Weerts Argonne National Laboratory.
SiD Tracking Simulation: Status and Plans Richard Partridge for the SiD Tracking Group Vancouver Linear Collider Workshop July 19-22, 2006.
Jerry Blazey May 31, 2007 LCWS07 1 SiD: Hadron Calorimetry Jerry Blazey Northern Illinois University LCWS07-Hamburg May 31, 2007.
SiD Concept – R&D Needs Andy White U. Texas at Arlington SiD Concept Meeting LCWS06 Bangalore, India March 11, 2006.
Silicon Tracking Systems in Mokka Framework Valeri Saveliev, Obninsk State University.
Summary of Simulation and Reconstruction Shaomin CHEN (Tsinghua University)  Framework and toolkit  Application in ILC detector design Jupiter/Satellites,
@ Future Plans for SiD & Opportunities for collaboration H.Weerts Argonne National Lab.
Preparing for the SiD LoI SiD Parallel Session TILC08 March 5, 2008 John Jaros.
International Workshop on Linear Colliders, Geneve Muon reconstruction and identification in the ILD detector N. D’Ascenzo, V.Saveliev.
1Frank Simon ALCPG11, 20/3/2011 ILD and SiD detectors for 1 TeV ILC some recommendations following experience from the CLIC detector study
SiD R&D tasks for the LOI - Subsystem R&D tasks - Summary of SiD R&D - Prioritization of R&D tasks -> Document for DoE/NSF ~Feb 2009 (Mainly based on Marty’s.
Performance and occupancies in a CCD vertex detector with endcaps Toshinori Abe and John Jaros 04/21/04.
CLICdp achievements in 2014 and goals for 2015 Lucie Linssen, CERN on behalf of the CLICdp collaboration CLIC workshop, January 30 th
Coil and HCAL Parameters for CLIC Solenoid and Hadron-calorimetry for a high energy LC Detector 15. December LAPP Christian Grefe CERN.
May 31th, 2007 LCWS C. Gatto 1 Tracking Studies in the 4 th Concept On behalf of 4th Concept Software Group D. Barbareschi V. Di Benedetto E. Cavallo.
Silicon Detector Tracking ALCPG Workshop Cornell July 15, 2003 John Jaros.
The Silicon Detector Concept Taipei ACFA Meeting November 9, 2004 John Jaros.
“Huge” Detector Concept 3 Sep 2004 ECFA LC Durham Satoru Yamashita ICEPP, University of Tokyo On behalf of many colleagues Towards our common.
ILC Calorimetry Test Beam Status Lei Xia ANL HEP.
How to Get Involved in SiD Richard Partridge Brown / SLAC LCWS 07.
Andrei Nomerotski, University of Oxford ILC VD Workshop, Menaggio 22 April 2008 SiD Vertex Detector.
LCWS11 – Tracking Performance at CLIC_ILD/SiD Michael Hauschild - CERN, 27-Sep-2011, page 1 Tracking Performance in CLIC_ILD and CLIC_SiD e + e –  H +
SiD Vertexing and Tracking Contribution to the LOI Bill Cooper Marcel Demarteau Ron Lipton Rich Partridge Dong Su For the SiD Vertex/Tracking Group SiD.
12/20/2006ILC-Sousei Annual KEK1 Particle Flow Algorithm for Full Simulation Study ILC-Sousei Annual KEK Dec. 20 th -22 nd, 2006 Tamaki.
Imaging Hadron Calorimeters for Future Lepton Colliders José Repond Argonne National Laboratory 13 th Vienna Conference on Instrumentation Vienna University.
SiD Tracking in the LOI and Future Plans Richard Partridge SLAC ALCPG 2009.
June 7, 2006SLAC DOE Review1 ILC Detector Detector for Silicon Detector for ILC SLAC DOE Program Review June 7, 2006 John Jaros.
VLCW06, July 23, 2006 H.Weerts Vancouver, CA 1 Where YOU can contribute in SiD. H.Weerts Argonne National Lab for SiD concept design study.
DESY1 Particle Flow Calorimetry At ILC Experiment DESY May 29 th -June 4 rd, 2007 Tamaki Yoshioka ICEPP, Univ. of Tokyo Contents.
Eunil Won/Korea U1 A study of configuration for silicon based Intermediate Trackers (IT) July Eunil Won Korea University.
Tracking: An Experimental Overview Richard Partridge Brown / SLAC Fermilab ALCPG Meeting.
Geant4-based detector simulation activities at NICADD Guilherme Lima for the NICADD simulations group December 2003.
Taikan Suehara, MEG collaboration Fukuoka, 23 Oct page 1 Taikan Suehara (Kyushu University) ILC detectors.
Intelligent Norman Graf, Steve Magill, Steve Kuhlmann, Ron Cassell, Tony Johnson, Jeremy McCormick SLAC & ANL CALOR ‘06 June 9, 2006 DesignDetector.
SiD R&D Plan and Opportunities for New Collaborators
SiD Calorimeter R&D Collaboration
A Silicon Detector for the ILC for the ILC – What is needed…
CLIC detector at SiD meeting 28/3/2010
The Compact Muon Solenoid Detector
Calorimetry for a CLIC experiment
State-of-the-art in Hadronic Calorimetry for the Lepton Collider
Detectors for Linear Colliders - ILC and CLIC -
Why do we want a TPC? P. Colas, CEA Saclay
Simulating the Silicon Detector
ILC Detector Technology
GEM-based Digital Hadron Calorimetry for SiD
Project Presentations August 5th, 2004
Detector Optimization using Particle Flow Algorithm
The LHCb Level 1 trigger LHC Symposium, October 27, 2001
Why do we want a TPC? P. Colas, CEA Saclay
Steve Magill Steve Kuhlmann ANL/SLAC Motivation
Sheraton Waikiki Hotel
Presentation transcript:

Jerry Blazey May 31, 2007 LCWS07 1 SiD Overview & Opportunities Jerry Blazey Northern Illinois University LCWS07-Hamburg June 1, 2007

Jerry Blazey May 31, 2007 LCWS07 2 The Challenge: Discovery & Precision Measurements Higgs & Recoil Mass Reconstruction (ie ZH) Higgs & Recoil Mass Reconstruction (ie ZH)  –excellent momentum resolution Higgs Decays Higgs Decays  –efficient b and c jet tags –precision di-jet mass (PFAs) to separate Ws and Zs SUSY Searches SUSY Searches  –hermiticity

Jerry Blazey May 31, 2007 LCWS07 3 VTX Tracker at minimum possible radius with max solid angle:VTX Tracker at minimum possible radius with max solid angle:  r  ~  rz = 5  10/p(sin 3/2  )  m Silicon strip tracker for excellent momentum resolution and robust performanceSilicon strip tracker for excellent momentum resolution and robust performance  p t /p t 2 ≤ 5 x GeV -1 Dense, highly segmented, Si-W Ecal and Hcal with a goal ofDense, highly segmented, Si-W Ecal and Hcal with a goal of  mjj =3-4% Instrumented flux return for muon identificationInstrumented flux return for muon identification The SiD Response Effort required to meet these ambitious goals …

Jerry Blazey May 31, 2007 LCWS07 4 SiD Details & Dimensions Vertex detector: 5 barrels, 4 disks; R in = 1.4 cm Si tracking: 5 layers; R in = 18 cm HCAL Fe: 34 layers; R in = 138 cm Solenoid: 5 T; R in = 250 cm EMCAL Si/W: 30 layers R in = 125 cm Flux return/muon R in = 333 cm R out = 645 cm Si PFA

Jerry Blazey May 31, 2007 LCWS07 5 Integrated Tracking: Pixel Vertex Detector & the Tracker VXD: standalone trackerVXD: standalone tracker –Space-point resolution < 4  m –Superb impact parameter resolution Five barrel layersFive barrel layers Four forward layersFour forward layers Transparency (~0.1% X 0 per layer)Transparency (~0.1% X 0 per layer) 14 mm from beam pipe14 mm from beam pipe Tracker: R i =0.22 m, R o =1.23 m, L= 3.3 mTracker: R i =0.22 m, R o =1.23 m, L= 3.3 m Five cylindersFive cylinders –tiled with 10x10cm 2 single sided microstrip sensors –Material budget 0.8% X 0 /layer Five (x2) endcap disksFive (x2) endcap disks –tiled with R,  microstrip sensors –Material budget 1.3% X 0 /layer

Jerry Blazey May 31, 2007 LCWS07 6 Tracking Performance Full simulationFull simulation Vertex detector seeded pattern recognition (3 hit combinations)Vertex detector seeded pattern recognition (3 hit combinations) Event SampleEvent Sample –ttbar-events –√s = 500 GeV –background included Black: VXD based Red: VXD + tracker ) ( 1 2  GeV p p T T  Efficiency CentralResolution

Jerry Blazey May 31, 2007 LCWS07 7 EM Calorimeter StatisticsStatistics –20/10 layers, 2.5/5 mm W –~ 1mm Si detector gaps –Tile with hexagonal 6” wafers –5x5 mm 2 pads –~ 1300 m 2 of Si Readout with KPIX chipReadout with KPIX chip –1024 channels, bump-bonded –4-deep buffer (low occupancy) –Bunch crossing time stamp for each hit CAD overview R 1.27 m  ->  +  o

Jerry Blazey May 31, 2007 LCWS07 8 HCAL Considerations BaselineBaseline –Gap size <~10mm –Barrel: mm SS absorbers  4  o –Two endcaps –Resistive Plate Chambers –Considering alternate technologies Resistive paint Mylar 1.2mm gas gap Mylar Aluminum foil 1.1mm glass - HV Signal pads -2100V ∆V ~400V 0V GEMs & Micromegas Scintillator/Solid State

Jerry Blazey May 31, 2007 LCWS07 9Solenoid Statistics:Statistics: –IR 2.5 m, OR 3.3 m –Length=5.4m –Stored Energy: 1.2GJ CMS-based feasibility study:CMS-based feasibility study: –Same conductor –CMS (4 layer)  SiD (6 layer) –CMS 5 modules 2.5 m long  SiD 2 modules 2.6 m long Uniformity good, stresses acceptable

Jerry Blazey May 31, 2007 LCWS07 10 Muon System Muon System Baseline ConfigurationMuon System Baseline Configuration –Octagon: 48 layers, 5 cm thick steel absorber plates –Six-Eight planes of x, y or u, v upstream of Fe flux return for xyz and direction of charged particles that enter muon system. Muon ID studiesMuon ID studies –12 RPC- instrumented gaps –~1cm spatial resolution IssuesIssues –Technology: RPC, Scin/SiPMs, GEMS, Wire chambers –Is the muon system needed as a tail catcher? –How many layers are needed (0-23)? Use HCAL ? –Position resolution needed? Muon Coil Hcal trackers Ecal End of HCal

Jerry Blazey May 31, 2007 LCWS07 11 Rewind: Technical Strengths Generally: compact, highly integrated, hermetic detectorGenerally: compact, highly integrated, hermetic detector Tracking:Tracking: –VTD: small radius ( 5T helps) –Tracker: excellent dp/p; minimized material all cos(  ) –Demonstrated pattern recognition –Solenoid: 5T (difficult but not unprecedented) Calorimetry: imaging, hermeticCalorimetry: imaging, hermetic –ECAL: excellent segmentation=4x4 mm 2, R Moliere =13mm –HCAL: excellent segmentation: ~1x1 to 3x3 cm 2 Excellent  ID: Instrumented flux return & imaging HCALExcellent  ID: Instrumented flux return & imaging HCAL

Jerry Blazey May 31, 2007 LCWS07 12Opportunities TrackingTracking –VTD technology –Forward System CalorimetryCalorimetry –Choice of HCAL technology requires study, PFA evaluation. Overall Optimization: Inner RadiusInner Radius Depth and Length?Depth and Length? B field?B field? –Forward systems challenging MuonMuon –Technology? –Layers? (Boost HCAL) Simulation & algorithmic toolsSimulation & algorithmic tools –Little mention –BUT there has been tremendous effort and many tools are in place)  Detector studies and MC benchmarking can be pursued!Detector studies and MC benchmarking can be pursued! Overall integration studies neededOverall integration studies needed

Jerry Blazey May 31, 2007 LCWS07 13 Looking Back a Bit & The Way Forward Silicon Detector Design Study Initiated Victoria ALCPG Meeting 2004Silicon Detector Design Study Initiated Victoria ALCPG Meeting 2004 Organization Fall-Winter ’04-’05Organization Fall-Winter ’04-’05 Progress on Technology, Simulation, Benchmarking, Cost ‘06Progress on Technology, Simulation, Benchmarking, Cost ‘06 Tools all in place for a workshop on optimization and choices, new ideas welcome – Fall ‘07.Tools all in place for a workshop on optimization and choices, new ideas welcome – Fall ‘07. Final choices – Spring ’08Final choices – Spring ’08 Letter of Intent – Summer ’08Letter of Intent – Summer ’08

Jerry Blazey May 31, 2007 LCWS07 14 Closing Comments A silicon-centric design offeringA silicon-centric design offering –unprecedented tracking precision –new potential in calorimetry –good muon identification Complementary to other conceptsComplementary to other concepts Many opportunities for new effort and expertise.Many opportunities for new effort and expertise. Tools and organization in place to support efficient development and to get started.Tools and organization in place to support efficient development and to get started. Great opportunity to explore ILC detector/physics.Great opportunity to explore ILC detector/physics. Open to new ideas, collaborators, increased internationalizationOpen to new ideas, collaborators, increased internationalization Rich Partridge will discuss interplay between physics/detector projects and avenues for involvement on SiD.Rich Partridge will discuss interplay between physics/detector projects and avenues for involvement on SiD.

Jerry Blazey May 31, 2007 LCWS07 15Organization EXECUTIVE COMMITTEE H.Aihara, J.Brau, M.Breidenbach, M.Demarteau, J.Jaros, J.Karyotakis, H.Weerts & A.White SOLENOID FLUX RET K.Krempetz VERY FORWARD W.Morse SIMULATION N.Graf MDI P.Burrows T.Markiewicz T.Tauchi VERTEXING Su Dong Ron Lipton Mech: W. Cooper CALORIMETERS A.White ECAL:R.Frey/D.Strom HCAL:G.Blazey/H.Weerts PFA:N.Graf/S.Magill MUON H.Band H.E.Fisk BENCHMARKING T.Barklow A.Juste COST M.Breidenbach R& D COORDINATOR A. White ADVISORY COMMITTEE All group leaders