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

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Presentation on theme: "Jerry Blazey May 31, 2007 LCWS07 1 SiD Overview & Opportunities Jerry Blazey Northern Illinois University LCWS07-Hamburg."— Presentation transcript:

1 http://www-sid.slac.stanford.edu/ Jerry Blazey May 31, 2007 LCWS07 1 SiD Overview & Opportunities Jerry Blazey Northern Illinois University LCWS07-Hamburg June 1, 2007

2 http://www-sid.slac.stanford.edu/ 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

3 http://www-sid.slac.stanford.edu/ 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 10 -5 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 …

4 http://www-sid.slac.stanford.edu/ 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

5 http://www-sid.slac.stanford.edu/ 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

6 http://www-sid.slac.stanford.edu/ 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

7 http://www-sid.slac.stanford.edu/ 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

8 http://www-sid.slac.stanford.edu/ Jerry Blazey May 31, 2007 LCWS07 8 HCAL Considerations BaselineBaseline –Gap size <~10mm –Barrel: 34 20-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

9 http://www-sid.slac.stanford.edu/ 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

10 http://www-sid.slac.stanford.edu/ 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

11 http://www-sid.slac.stanford.edu/ 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

12 http://www-sid.slac.stanford.edu/ 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

13 http://www-sid.slac.stanford.edu/ 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

14 http://www-sid.slac.stanford.edu/ 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.

15 http://www-sid.slac.stanford.edu/ 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


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