SVD upgrade for sbelle
|
|
- Hugo Barnett
- 5 years ago
- Views:
Transcription
1 SVD upgrade for sbelle T.Kawasaki(Niigata-U) Mar19-20, 2008 Super Belle Pre kick-off 1
2 Requirements for sbelle Tracker 1. More tracking efficiency High precision measurement with high statistics to search the new physics in B decays B B 0 0 φk K S 0, ηk 0 π γ 0, K S K S K (tcpv) B τν, μν, Dτν Hermeticity τ μγ S (tcpv) Ks vertexing High Hermeticity/Acceptance coverage Good efficiency on Low momentum & Ks daughter tracking, Mar19-20, 2008 Super Belle Pre kick-off 2
3 Requirements for sbelle Tracker 2. Robust against high beam background We assume Occ first layer of Belle SVD(r=2cm) Fine segmentation Fast pulse shaping & time slice information High trigger rate Need high speed & deadtime free readout Hit finding eff. Belle 34 15% Occupancy By Fujiyama(TIT) 3. Better Resolution (At least competitive performance as current SVD) Thin sensor Momentum resolution Small BP radius Impact parameter and vertex resolution Mar19-20, 2008 Super Belle Pre kick-off 3
4 Aim 1cm radius beam pipe Super Belle Vertex Tracker (LoI 04 for SuperB) (cm) Two thin pixel layers r =150mm 17 6 sensor layers to make low momentum tracking Slanted layer to keep acceptance, optimize incident angle and save detector size (cm) Mar19-20, 2008 Super Belle Pre kick-off 4
5 Upgrade Schedule Along to the current upgrade schedule Stop Belle R&D KEKB&Belle upgrade Start sbelle Stop Belle on the end of 2008 (JPY) Start sbelle operation from the beginning of 2012 Reconstruction of detector takes 3 years We have only 1 year for R&D work!! We need REALISTIC upgrade plan for T=0 operation in 2012 ( with ~10 35 ) Further upgrade can be done after getting higher luminosity (1cm beampipe, Thin Monolithic Pixel sensor needs further R&D work) Mar19-20, 2008 Super Belle Pre kick-off 5
6 Occupancy estimation Occupancy estimation (L=2x10^35, x20 BG, 10kHz trigger rate) Assuming Occ Tp, channel area, 1/r 2 Current SVD VA1(Tp=800ns): ~8%@ 1 st layer L = % 20BG = 160%! Ex)APV25 (developed for CMS Si Tracker) Tp=50ns Factor 16 reduction is possible Shaper 160 pipeline FIFO pulse shape scan with 40MHz Clk Further BG reduction is possible by Pulse shape and timing information 32 step FIFO as event queues Deadtime free readout@ 10kHz trigger rate ns Standard rectangle DSSD is OK Mar19-20, 2008 Super Belle Pre kick-off 6
7 The current detector (SVD2) Size of DSSD R [mm] Z [mm] [mm 2 ] st x nd x rd x th x73.8 Beam Pipe DSSD in z ladde r in φ SVD3: Replace L1 (&L2) with similar ladders readout with APV25. Proposed as intermediate upgrade plan. We are the final stage of mass production. Postponed (?) if sbelle construction really start in Mar19-20, 2008 Super Belle Pre kick-off 7
8 Realistic deliberation for 2x10 35 SVD2 Nonsense! Performance SVD3 Minimal fallback 4layer, r=1.5cm(same as SVD2) Low Replace L1,2 of SVD2 with APV(fast shaping) Keep SVD2 L3,4(slow shaping~1μs, 30μs deadtime) Budget Cheap SVD3Mod Baseline (Day 0 for 2x10^35) 4~6 layer, r=1.5cm L5&6: Thick material; 500μm-t <=Chip on sensor, Slant (cone/disk) FW/BW All layer readout with fast shaping~50ns High SuperVTX Ideal (further upgrade ~2015 toward 10^36?) 6 layer, r=1cm, L5,6: FW L1,2: Thin Pixel(~50μm ) L3~6: DSSD with Short Tp Expensive Mar19-20, 2008 Super Belle Pre kick-off 8
9 SVD(SVT) upgrade Strategy T=0 option (2012) for L = ~ Keep beampipe radius of 1.5cm same as current one Current SVD configuration + 2 outer layers = 6 layers Improve Ks efficiency. Replace CDC inner layers Similar design DSSD can be used Fast Shaping(~50ns) + Timeslice on FE chip Further upgrade for L >10 35 Smaller beampipe radius (r =1cm or less) Innermost (thin) Pixel layers Improve impact parameter resolution Mar19-20, 2008 Super Belle Pre kick-off 9
10 x30bg ~10 36 Occupancy estimation Assuming SVD3 x15bg SVD3mod <1 2x10 35 SuperVTX <1 <1 3 1 <1 SVD3 SVD3mod SuperVTX L <1 L <1 L Int res = x1.5(1.2) for 30%(10%) occupancy Occupancy 1/r 2 sensor aread Hit efficiency loss is not considered. (-10% for 30% Occ) 2 6 L L5 - - <1 1 L6 - <1 <1 - <1 1 Deadtime ~60% negligble negligble?? ~5%? ~5%? [%] 10kHz trigger rate Mar19-20, 2008 Super Belle Pre kick-off 10
11 To be discussed Configuration/Design To be discussed and fixed by the end of 2009 More MC study is needed Mentioned later Technology choice Depend on budget/time/man power What technology should be developed? Concentrate to the selected items Mentioned later Mar19-20, 2008 Super Belle Pre kick-off 11
12 Configuration/Design Layer positions in r IP resolution (beampipe and 1 st layer) Momentum resolution Tracking efficiency for low p track and Ks. Material budget Inner Layer IP resolution Outer Layer momentum resolution All items are not fixed yet Strip pitch on outer layer Fine pitch: Good resolution Wide Pitch: S/N, #readout Slant part Acceptance, hermeticity, optimize incident angle Reduce #readout Mar19-20, 2008 Super Belle Pre kick-off 12
13 Study on Detector configuration SVD r = 2.0, 4.35, 7.0, 8.8 cm CDC r= 8.8 ~ 86.3cm SVD Add r = (13), 14cm CDC r=16.0 ~ 112.0cm Belle CDC CDC sbelle Put 5&6 layer SVD SVD Evaluate new detector configuration with TRACKERR calculation & GEANT3 full simulation Modify the current Belle simulator Use L4 ladder structure as L5&6 layer No sensor at forward region Mar19-20, 2008 Super Belle Pre kick-off 13
14 Ks reconstruction : 5 th layer position 0 B * 0 K ( KSπ )γ GEANT3 Eff. Ks Ks Vtx resolution Full simulation by Shinomiya (Osaka) Require SVD hits on 2 layers sin 2φ eff 1 =0.68 Move 5 th layer to outer More Ks but poor B vtx resolution Ks B vertex: Ks pseudo track + Beam profile Relative luminosity to measure Acp e - e + Beam profile Mar19-20, 2008 Super Belle Pre kick-off 14
15 Impact Parameter resolution [cm] 0.02 r-φ direction [cm] 0.03 Calculated by TRACKERR z direction LoI 04 sbelle SVD2(now) 0.01 For π 0.2GeV 0.5GeV 1.0GeV 2.0GeV Beampipe radius is important Competitive performance as the current SVD sinθ Occupancy effects. Degradation of intrinsic resolution is included. Efficiency loss is NOT included Mar19-20, 2008 Super Belle Pre kick-off 15
16 Momentum IP [rad] 0.02 φ resolution [/MeV] 0.3 κ resolution Calculated by TRACKERR LoI 04 sbelle SVD2(now) For π 0.2GeV 0.5GeV 1.0GeV 2.0GeV sinθ Competitive performance as the current SVD More layer doesn t worsen momentum resolution Mar19-20, 2008 Super Belle Pre kick-off 16
17 T.Hara(Osaka) Res. Center value Mar19-20, 2008 Super Belle Pre kick-off 17
18 Requirement on S/N ratio Assuming Si Noise determined by Sensor Leakage current Detector Capacitance 3DSSDs are readouted via FLEX Chain readout makes large detector capacitance Noise performance depends on FE chip Belle Tp = 1μs enc [e - ]= /Cd[pF] Leakage current dominates 3DSSDs:~60pF 630e esBelle Tp = 50ns enc [e - ]= /Cd[pF] Detector capacitance is crucial (calculate Cd component only) Mar19-20, 2008 Super Belle Pre kick-off 18
19 Effect of poor S/N ratio on the outer layers M.E. (Matching Efficiency) = Prob.(SVD hits are found on at least 2 SVD layers) GEANT3 Full sim. M.E. Increase noise M.E. CDC SVT All Layers Noise 10 Typ. Only 5&6 Layers Noise 10 Typ. Kalman filtering Extrapolate track from CDC S/N degradation on the outer layer doesn t affect to M.E. so much But, In case of Ks daughter track Mar19-20, 2008 Super Belle Pre kick-off 19
20 Matching efficiency for Ks + π + B K S SVD Matched track L3 L4 L5 Increase Noise on L5&L6 only L3 L4 GEANT3 Full sim By Nakagawa (Niigata) L5 r of Ks decay vertex r of Ks decay vertex M.E. for Ks daughters are affected by S/N degradation Lose 20% (SVT) events with 4 times worse S/N Mar19-20, 2008 Super Belle Pre kick-off 20
21 Change thresholds on SVD hit finding Noise x 3 Threshold = 3 x σ Default setting Threshold = 2 x σ Lower thresholds save Matching efficiency. But lower thresholds make data size huge Mar19-20, 2008 Super Belle Pre kick-off 21
22 Key technology for upgrade Timeslice Information/Full Pipeline readout Pipeline in FE chip (APV25, VA-modified, own ASIC) Practical implementation scheme in a limited space Ladder assembling. Mechanical Support structure Cooling/Cabling scheme Save S/N for outer layer. FLEX readout. Chip on sensor Sensor development Low noise & Large area sensor is desirable Thin (less material) Thick (more signal) Pixel sensor (Option for future upgrade) Thin & Fast readout. Monolithic device? No more HPK DSSD. Micron? SINTEF? New activities started by India/Korea group Mar19-20, 2008 Super Belle Pre kick-off 22
23 R&D activities We have been working to prepare Pipeline readout sensor module for SVD3 Hybrid card with 4 APV25 chips Operated with 40MHz clock (Princeton) FADC: 40MHz digitization Online sparsification with FPGA (Vienna) Beamtest done in KEK in Nov 2007 in KEK Fuji testbeam line 3GeV electron Confirm the capability of online sparsification algorithm The result will come soon Mar19-20, 2008 Super Belle Pre kick-off 23
24 Chip on sensor with FLEX hybrid Keep good S/N ratio at the outer layers Proposal by Vienna group Readout each DSSD by putting thinned FE chip on sensor Cooling with water through carbon fiber tube (low material and good thermal conduction) No Cooling Cooling with 13 water Mar19-20, 2008 Super Belle Pre kick-off 24
25 Schedule Assuming that all R&D items are performed and finished in time. It is too dangerous scenario. We should concentrate on selected items. Mar19-20, 2008 Super Belle Pre kick-off 25
26 Schedule for SVT upgrade Stop Belle We are here Start sbelle SVT Design R&D Sensor Production Endring &Beampipe Assembling Test Installation Final Test NOT official one Mar19-20, 2008 Super Belle Pre kick-off 26
27 Summary We start the activity for SVD upgrade for sbelle Any activities and contributions are welcome. Please join! Requirements on new SVD(SVT?) In my opinion, we should keep current resolution and improve acceptance and efficiency. Configuration/Design Please feel free to propose new idea. Nothing is decided yet. Technology Please propose your idea. But be aware on tight schedule and budget.. Mar19-20, 2008 Super Belle Pre kick-off 27
28 Extended meeting for SVD upgrade on Feb20 You need to know account for KEK indico page Mar19-20, 2008 Super Belle Pre kick-off 28
29 Backups Mar19-20, 2008 Super Belle Pre kick-off 29
30 Condition Start sbelle on 2012 Start Construction in 2009 Budget is limited (not determined yet) We should have some options Luminosity & Background L=2x10^35, x20 BG, 10kHz trigger rate. Keep current performance on resolution Improve efficiency Acceptance, hermeticity, Ks eff., Slow tracking. My own Mar19-20, 2008 Super Belle Pre kick-off 30
31 Online Sparsification at SVD readout Processing with 500~1kHz Online Offline SVD FADC Online PCFARM Storage Analysis Clustering Data sparsification for each strip. Threshold = 3.7 σ Noise is calculated as σ of pedestal Threshold = 3. x σ It is difficult to set low threshold since lower thre. Make data size huge. Mar19-20, 2008 Super Belle Pre kick-off 31
32 Other activity New DSSD company No longer HPK DSSD Micron sensor will be evaluated Will be delivered by the end of March. India/Korea group Working to develop high performance DSSD independently Development of FE Readout chip APV25 was designed 10 years ago. Hawaii group started the design of own FE readout chip Pipeline on each channel. Hopefully, short shaping time ~ 50ns and good noise performance Krakow has also interests Develop pipeline VA chip with IDEAS? Mar19-20, 2008 Super Belle Pre kick-off 32
33 Readout scheme Mar19-20, 2008 Super Belle Pre kick-off 33
34 Ladder structure/ Cabling.. Mar19-20, 2008 Super Belle Pre kick-off 34
35 Super Belle detector (LoI 04) SC solenoid 1.5T μ / K L detection 14/15 lyr. RPC+Fe tile scintillator CsI(Tl) 16X 0 pure CsI (endcap) Aerogel Cherenkov counte + TOF counter TOP + RICH New readout and computing systems Si vtx. det. 4 lyr. DSSD 2 pixel/striplet lyrs. + 4 lyr. DSSD Tracking + de/dx small cell + He/C 2 H 6 remove inner lyrs. use fast gas Mar19-20, 2008 Super Belle Pre kick-off 35
36 Mar19-20, 2008 Super Belle Pre kick-off 36
37 Material effect Mar19-20, 2008 Super Belle Pre kick-off 37
38 Sensor Configuration (SVD1 SVD2) SVD2) 45cm 22cm Z view 46cm Mar19-20, 2008 Super Belle Pre kick-off 38
39 BG effect on physics analysis J / ψ ( μμ) K Nominal 5 BG 20 BG 20 BG Preliminary S B Eff 56.8 % 56.0 % 49.0 % % With 40% shorter shaping 51.4 % ( π Total performance of CDC + SVD + π ) Ratio % -1.5 % -9.5 % ( D Dπ,D K 3π ) Major loss comes from low tracking efficiency for slow particles Efficiency loss on high multiplicity event is serious Moreover a pulse shape information CDC by FADC readout can save efficiency Gain by SVD standalone tracker is not included D * D * Nominal 5 BG 20 BG 20 BG * B Eff 6.48% 5.69% 2.28% With 40% shorter shaping 3.86% s Ratio % % % % By Ozaki Mar19-20, 2008 Super Belle Pre kick-off 39
40 Intrinsic Resolution vs. Occupancy Intrinsic Resolution occupancy < 0.04 occupancy residual [ m[ residual residual [ m[ residual At high occupancy, cluster shape is 'distorted' reconstructed cluster energy to be off the residual distribution to be widened Occupancy S.Fratina Mar19-20, 2008 Super Belle Pre kick-off 40
41 Hit Efficiency vs. Occupancy Layer No. Efficiency hit or not? Layer1 2 Layer2 Higher Occupancy ~ Lower Hit Efficiency Signal + background hits wider 'distorted' cluster 0.6 Layer3 3 Layer4 4 0% 30% Occupancy Wrongly associated background cluster Mar19-20, 2008 Super Belle Pre kick-off 41 Y.Fujiyama
42 Occupancy problem at innermost layer Estimate occupancy at Super B Occupancy at SVD2 At most, 10% in r =20mm for /cm 2 /s Assuming Occ. = luminosity/r 2 r =15mm for /cm 2 /s occupancy = 200% Factor 40 of reduction is needed!! How can we reduce Occ.? Assuming Occ. = sensitive area* shaping time Short shaping time Tp=100ns is possible (Factor 8) (SVD2:VA1TA, Tp=800ns) Strip area should be small. Area=pitch*length short strip How to shorten a strip length by 1/5? % 1 L=10 35 /cm 2 /s Occupancy (%) SVD1(1usec) SVD2(500nsec) SVD2(800nsec) Radius (cm) Mar19-20, 2008 Super Belle Pre kick-off 42
43 Striplet design To shorten strip length, we propose new type of DSSD Arrange strips in 45 degrees. Strip length is shortened Small triangle dead region exists. About 7 % in Layer1 Z rφ Striplet can survive up to /cm 2 /s (10 36 needs pixel type sensor!) 10mm Occupancy (%) 70mm Mar19-20, 2008 Super Belle Pre kick-off % Dead region Striplet Tp=50ns SVD1(1usec) SVD2(500nsec) SVD2(800nsec) S-VTX(50nsec) S-VTX(100nsec) With striplet Radius (cm) mm U V
44 Prototype Striplet Sensor (HPK) 2.75mm 74.1mm 71.0 mm Thickness:300μm Double sided P and N strips on N-bulk Incline strip by 45 degree strips on each side 10.5mm 8.5mm Strip pitch = 51μm in U-V direction. (Pad spacing is 72μm along sensor edge) Since sensor size is small, inactive region can t be ignored How to reduce dead region Check behavior near inactive region carefully. Mar19-20, 2008 Super Belle Pre kick-off 44
45 Scan strips with IR laser scan Results Striplet detector is functional. No signal on the triangle part The edge of active region is so sharp. Signal (normalized) P-side sum Signal (normalized) N-side End of active region sum Laser position[μm] Laser position[μm] Mar19-20, 2008 Super Belle Pre kick-off 45
46 全層の S/N を悪くしたとき Matching efficiency Normal S/N Noise x 4 Noise x 5 Mar19-20, 2008 Super Belle Pre kick-off 46
47 Matching efficiency for the various threshold. Default noise Noise = default x 2 Mar19-20, 2008 Super Belle Pre kick-off 47
48 Noise = default x 3 Noise = default x 4 Mar19-20, 2008 Super Belle Pre kick-off 48
49 Noise = default x 5 Mar19-20, 2008 Super Belle Pre kick-off 49
50 Mis-alignment effect Large VTX tracker makes difficulty on alignment. Ks eff. Ks VTX Resolution Red: Perfectly aligned Blue: 10um, 0.1mrad Green: 20um, 0.2mrad Pink: 30um, 0.3mrad Mis-alignment doesn t affect to efficiency Mar19-20, 2008 Super Belle Pre kick-off 50
51 Hit timing reconstruction B-Factory --> 2 nsec bunch crossing APV25 deconvolution filter can not be used. Hit time reconstruction Proposed by Vienna group Read out 3, 6 slices in the pipeline for one trigger. Extract the hit timing information from wave form. Trigger Shaper Proven in beam tests: Resolution ~ 2 nsec. Reconstruction done in the FPGA chips in FADC board. (HEPHY Vienna) Mar19-20, 2008 Super Belle Pre kick-off 51 The silicon tracker development at KEK, Toru TSuboyama (KEK), 19 Dec SILC meeting at Torino, Italy 51
52 Mar19-20, 2008 Super Belle Pre kick-off 52
53 Mar19-20, 2008 Super Belle Pre kick-off 53
The Belle Silicon Vertex Detector. T. Tsuboyama (KEK) 6 Dec Workshop New Hadrons with Various Flavors 6 7 Dec Nagoya Univ.
The Belle Silicon Vertex Detector T. Tsuboyama (KEK) 6 Dec. 2008 Workshop New Hadrons with Various Flavors 6 7 Dec. 2008 Nagoya Univ. Outline Belle Silicon vertex detector Upgrade plan R&D and beam tests
More informationThe Silicon Vertex Detector of the Belle II Experiment
Thomas Bergauer (HEPHY Vienna) 12th Pisa Meeting on Advanced Detectors Belle and Belle II DEPFET Pixel Detector Double-sided Strip Detector Summary Thomas Bergauer 2 KEKB and Belle @ KEK (1999-2010) KEKB
More informationEndcap Modules for the ATLAS SemiConductor Tracker
Endcap Modules for the ATLAS SemiConductor Tracker RD3, Firenze, September 29 th, 23 Richard Nisius (MPI Munich) nisius@mppmu.mpg.de (For the ATLAS-SCT Collaboration) The plan of this presentation Introduction
More informationCourse Updates. Reminders: 1) Assignment #12 due today. 2) Polarization, dispersion. 3) Last HW (#13 posted) due Monday, May 3rd
Course Updates http://www.phys.hawaii.edu/~varner/phys272-spr10/physics272.html Reminders: 1) Assignment #12 due today 2) Polarization, dispersion 3) Last HW (#13 posted) due Monday, May 3rd n 1 n 2 Total
More informationThe LHCb upgrade. Outline: Present LHCb detector and trigger LHCb upgrade main drivers Overview of the sub-detector modifications Conclusions
The LHCb upgrade Burkhard Schmidt for the LHCb Collaboration Outline: Present LHCb detector and trigger LHCb upgrade main drivers Overview of the sub-detector modifications Conclusions OT IT coverage 1.9
More informationBeam test measurements of the Belle II vertex detector modules
Beam test measurements of the Belle II vertex detector modules Tadeas Bilka Charles University, Prague on behalf of the Belle II Collaboration IPRD 2016, 3 6 October 2016, Siena, Italy Outline Belle II
More informationPXD Simulation and Optimisation Studies
PXD Simulation and Optimisation Studies Z. Drásal, A. Moll, K. Prothmann with special thanks to: C. Kiesling, A. Raspereza, Prague people Charles University Prague MPI Munich ILC Software Framework Summary
More informationATLAS ITk Layout Design and Optimisation
ATLAS ITk Layout Design and Optimisation Noemi Calace noemi.calace@cern.ch On behalf of the ATLAS Collaboration 3rd ECFA High Luminosity LHC Experiments Workshop 3-6 October 2016 Aix-Les-Bains Overview
More informationPerformance of FPCCD vertex detector. T. Nagamine Tohoku University Feb 6, 2007 ACFA 9, IHEP,Beijin
Performance of FPCCD vertex detector T. Nagamine Tohoku University Feb 6, 27 ACFA 9, IHEP,Beijin Outline FPCCD and Vertex Detector Structure Impact Parameter Resolution Pair Background in Vertex Detector
More informationFirst Operational Experience from the LHCb Silicon Tracker
First Operational Experience from the LHCb Silicon Tracker 7 th International Hiroshima Symposium on Development and Application of Semiconductor Tracking Devices The LHCb Silicon Tracker Installation
More informationA proximity focusing RICH with time-of-flight capabilities
A proximity focusing RICH with time-of-flight capabilities Peter Križan University of Ljubljana and J. Stefan Institute For the Belle Aerogel RICH R&D group 10th Topical Seminar on Innovative Particle
More informationThe Phase-2 ATLAS ITk Pixel Upgrade
The Phase-2 ATLAS ITk Pixel Upgrade T. Flick (University of Wuppertal) - on behalf of the ATLAS collaboration 14th Topical Seminar on Innovative Particle and Radiation Detectors () 03.-06. October 2016
More informationPerformance of the ATLAS Inner Detector at the LHC
Performance of the ALAS Inner Detector at the LHC hijs Cornelissen for the ALAS Collaboration Bergische Universität Wuppertal, Gaußstraße 2, 4297 Wuppertal, Germany E-mail: thijs.cornelissen@cern.ch Abstract.
More informationFirst results from the LHCb Vertex Locator
First results from the LHCb Vertex Locator Act 1: LHCb Intro. Act 2: Velo Design Dec. 2009 Act 3: Initial Performance Chris Parkes for LHCb VELO group Vienna Conference 2010 2 Introducing LHCb LHCb is
More informationIntegrated CMOS sensor technologies for the CLIC tracker
Integrated CMOS sensor technologies for the CLIC tracker Magdalena Munker (CERN, University of Bonn) On behalf of the collaboration International Conference on Technology and Instrumentation in Particle
More informationProduction and Quality Assurance of Detector Modules for the LHCb Silicon Tracker
Production and Quality Assurance of Detector Modules for the LHCb Silicon Tracker Olaf Steinkamp for Dmytro Volyanskyy Physik-Institut der Universität Zürich 10th ICATPP Conference on Astroparticle, Particle,
More informationSiPMs for Čerenkov imaging
SiPMs for Čerenkov imaging Peter Križan University of Ljubljana and J. Stefan Institute Trends in Photon Detectors in Particle Physics and Calorimetry, Trieste, June 2-4, 2008 Contents Photon detectors
More informationSiD VXD Conceptual Design Su Dong SLAC
SiD VXD Conceptual Design Su Dong SLAC Aug/23/05 Su Dong Snowmass 05 VTX WG: SiD VXD conceptual Design 1 Common Design Features Like other detector concepts, SiD VXD design is open to all sensor technology
More informationExpected feedback from 3D for SLHC Introduction. LHC 14 TeV pp collider at CERN start summer 2008
Introduction LHC 14 TeV pp collider at CERN start summer 2008 Gradual increase of luminosity up to L = 10 34 cm -2 s -1 in 2008-2011 SLHC - major increase of luminosity up to L = 10 35 cm -2 s -1 in 2016-2017
More informationThe CMS Tracker Laser Alignment System
The CMS Tracker Laser Alignment System B.Wittmer, I. Physikalishes Institut RWTH Aachen on behalf of the CMS Tracker collaboration Vertex 9 Workshop, Putten (NL) 1 Outline Working Principle and Layout
More informationTHE ATLAS INNER DETECTOR OPERATION, DATA QUALITY AND TRACKING PERFORMANCE.
Proceedings of the PIC 2012, Štrbské Pleso, Slovakia THE ATLAS INNER DETECTOR OPERATION, DATA QUALITY AND TRACKING PERFORMANCE. E.STANECKA, ON BEHALF OF THE ATLAS COLLABORATION Institute of Nuclear Physics
More informationarxiv: v1 [physics.ins-det] 13 Dec 2018
Millepede alignment of the Belle 2 sub-detectors after first collisions arxiv:1812.05340v1 [physics.ins-det] 13 Dec 2018 Tadeas Bilka, Jakub Kandra for the Belle II Collaboration, Faculty of Mathematics
More informationStefania Beolè (Università di Torino e INFN) for the ALICE Collaboration. TIPP Chicago, June 9-14
ALICE SDD ITS performance with pp and Pb-Pb beams Stefania Beolè (Università di Torino e INFN) for the ALICE Collaboration - Chicago, June 9-14 Inner Tracking System (I) Six layers of silicon detectors
More informationCharged Particle Tracking at Cornell: Gas Detectors and Event Reconstruction
Charged Particle Tracking at Cornell: Gas Detectors and Event Reconstruction Dan Peterson, Cornell University The Cornell group has constructed, operated and maintained the charged particle tracking detectors
More informationCMS FPGA Based Tracklet Approach for L1 Track Finding
CMS FPGA Based Tracklet Approach for L1 Track Finding Anders Ryd (Cornell University) On behalf of the CMS Tracklet Group Presented at AWLC June 29, 2017 Anders Ryd Cornell University FPGA Based L1 Tracking
More informationOptimisation Studies for the CLIC Vertex-Detector Geometry
CLICdp-Note04-002 4 July 204 Optimisation Studies for the CLIC Vertex-Detector Geometry Niloufar Alipour Tehrani, Philipp Roloff CERN, Switzerland, ETH Zürich, Switzerland Abstract An improved CLIC detector
More informationDesign of the new ATLAS Inner Tracker (ITk) for the High Luminosity LHC
Design of the new ATLAS Inner Tracker (ITk) for the High Luminosity LHC Jike Wang (DESY) for the ATLAS Collaboration May/2017, TIPP 2017 LHC Machine Schedule In year 2015, ATLAS and CMS went into Run2
More informationDetector R&D at the LCFI Collaboration
LCFI Overview Detector R&D at the LCFI Collaboration (Bristol U, Oxford U, Lancaster U, Liverpool U, RAL) Konstantin Stefanov on behalf of the LCFI collaboration LCWS2005, Stanford, 18-22 March 2005 Introduction
More informationTORCH: A large-area detector for precision time-of-flight measurements at LHCb
TORCH: A large-area detector for precision time-of-flight measurements at LHCb Neville Harnew University of Oxford ON BEHALF OF THE LHCb RICH/TORCH COLLABORATION Outline The LHCb upgrade TORCH concept
More informationPerformance of the GlueX Detector Systems
Performance of the GlueX Detector Systems GlueX-doc-2775 Gluex Collaboration August 215 Abstract This document summarizes the status of calibration and performance of the GlueX detector as of summer 215.
More informationGEANT4 is used for simulating: RICH testbeam data, HCAL testbeam data. GAUSS Project: LHCb Simulation using GEANT4 with GAUDI.
Status of GEANT4 in LHCb S. Easo, RAL, 30-9-2002 The LHCbexperiment. GEANT4 is used for simulating: RICH testbeam data, HCAL testbeam data. GAUSS Project: LHCb Simulation using GEANT4 with GAUDI. Summary.
More informationOverview of the American Detector Models
Overview of the American Detector Models Univ. of Oregon The American study groups have investigated two specific models Choosing any particular detector design is a compromise between competing constraints
More informationThe CLICdp Optimization Process
ILDOptWS, Feb, 2016 A. Sailer: The CLICdp Optimization Process 1/17 The CLICdp Optimization Process André Sailer (CERN-EP-LCD) On Behalf of the CLICdp Collaboration ILD Software and Optimisation Workshop
More informationSimulating the RF Shield for the VELO Upgrade
LHCb-PUB-- March 7, Simulating the RF Shield for the VELO Upgrade T. Head, T. Ketel, D. Vieira. Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil European Organization for Nuclear Research
More informationTrack reconstruction for the Mu3e experiment based on a novel Multiple Scattering fit Alexandr Kozlinskiy (Mainz, KPH) for the Mu3e collaboration
Track reconstruction for the Mu3e experiment based on a novel Multiple Scattering fit Alexandr Kozlinskiy (Mainz, KPH) for the Mu3e collaboration CTD/WIT 2017 @ LAL-Orsay Mu3e Experiment Mu3e Experiment:
More informationModules and Front-End Electronics Developments for the ATLAS ITk Strips Upgrade
Modules and Front-End Electronics Developments for the ATLAS ITk Strips Upgrade Carlos García Argos, on behalf of the ATLAS ITk Collaboration University of Freiburg International Conference on Technology
More informationCharged particle detection performances of CMOS Pixel Sensors designed in a 0.18 µm CMOS process based on a high resistivity epitaxial layer
Charged particle detection performances of CMOS Pixel Sensors designed in a 0.18 µm CMOS process based on a high resistivity epitaxial layer Jérôme Baudot on behalf of the PICSEL team of IPHC-Strasbourg
More informationNew results from LDCPrime optimization studies
New results from LDCPrime optimization studies with the Vienna Fast Simulation Tool ( LiC Detector Toy ) The Vienna Fast Simulation Tool LDT Simple, but flexible and powerful tool Version 2.0 available
More informationarxiv:physics/ v1 [physics.ins-det] 18 Dec 1998
Studies of 1 µm-thick silicon strip detector with analog VLSI readout arxiv:physics/981234v1 [physics.ins-det] 18 Dec 1998 T. Hotta a,1, M. Fujiwara a, T. Kinashi b, Y. Kuno c, M. Kuss a,2, T. Matsumura
More informationThe LHCb Upgrade. LHCC open session 17 February Large Hadron Collider Physics (LHCP) Conference New York, 2-7 June 2014
The LHCb Upgrade LHCC open session 17 February 2010 Large Hadron Collider Physics (LHCP) Conference New York, 2-7 June 2014 Andreas Schopper on behalf of Motivation LHCb is a high precision experiment
More informationCharged Particle Tracking at Cornell: Gas Detectors and Event Reconstruction
Charged Particle Tracking at Cornell: Gas Detectors and Event Reconstruction Dan Peterson, Cornell University The Cornell group has constructed, operated and maintained the charged particle tracking detectors
More informationTrack reconstruction with the CMS tracking detector
Track reconstruction with the CMS tracking detector B. Mangano (University of California, San Diego) & O.Gutsche (Fermi National Accelerator Laboratory) Overview The challenges The detector Track reconstruction
More informationConstruction of the Phase I upgrade of the CMS pixel detector
Forward Pixel Barrel Pixel TECHNOLOGY AND INSTRUMENTATION IN PARTICLE PHYSICS 2017, May 22-26, 2017 Construction of the Phase I upgrade of the CMS pixel detector Satoshi Hasegawa Fermi National Accelerator
More informationSimulation study for the EUDET pixel beam telescope
EUDET Simulation study for the EUDET pixel beam telescope using ILC software T. Klimkovich January, 7 Abstract A pixel beam telescope which is currently under development within the EUDET collaboration
More informationTPC Detector Response Simulation and Track Reconstruction
TPC Detector Response Simulation and Track Reconstruction Physics goals at the Linear Collider drive the detector performance goals: charged particle track reconstruction resolution: δ(1/p)= ~ 4 x 10-5
More informationThe performance of the ATLAS Inner Detector Trigger Algorithms in pp collisions at the LHC
X11 opical Seminar IPRD, Siena - 7- th June 20 he performance of the ALAS Inner Detector rigger Algorithms in pp collisions at the LHC Mark Sutton University of Sheffield on behalf of the ALAS Collaboration
More informationEicRoot for tracking R&D studies
EicRoot for tracking R&D studies Alexander Kiselev EIC Software Meeting Jefferson Lab September,24 2015 Contents of the talk Tracking code implementation in EicRoot Few particular applications: Basic forward
More informationThe LHCb VERTEX LOCATOR performance and VERTEX LOCATOR upgrade
Journal of Instrumentation OPEN ACCESS The LHCb VERTEX LOCATOR performance and VERTEX LOCATOR upgrade To cite this article: P Rodríguez Pérez Related content - Upgrade of the LHCb Vertex Locator A Leflat
More informationfor the DESY/ ECFA study detector
The TPC Tracker for the DESY/ ECFA study detector Ties Behnke DESY 1-May-1999 the TPC tracker requirements from physics a TPC at TESLA: can this work? results from simulation technical issues conclusion
More informationATLAS Dr. C. Lacasta, Dr. C. Marinas
ATLAS Dr. C. Lacasta, Dr. C. Marinas cmarinas@uni-bonn.de 1 http://www.atlas.ch/multimedia/# Why? In particle physics, the processes occur on a scale that is either too brief or too small to be observed
More informationarxiv:hep-ph/ v1 11 Mar 2002
High Level Tracker Triggers for CMS Danek Kotliński a Andrey Starodumov b,1 a Paul Scherrer Institut, CH-5232 Villigen, Switzerland arxiv:hep-ph/0203101v1 11 Mar 2002 b INFN Sezione di Pisa, Via Livornese
More informationEUDET Telescope Geometry and Resolution Studies
EUDET EUDET Telescope Geometry and Resolution Studies A.F.Żarnecki, P.Nieżurawski February 2, 2007 Abstract Construction of EUDET pixel telescope will significantly improve the test beam infrastructure
More informationCharged Particle Reconstruction in HIC Detectors
Charged Particle Reconstruction in HIC Detectors Ralf-Arno Tripolt, Qiyan Li [http://de.wikipedia.org/wiki/marienburg_(mosel)] H-QM Lecture Week on Introduction to Heavy Ion Physics Kloster Marienburg/Mosel,
More informationAlignment of the ATLAS Inner Detector tracking system
Alignment of the ATLAS Inner Detector tracking system Instituto de Física Corpuscular (IFIC), Centro Mixto UVEG-CSIC, Apdo.22085, ES-46071 Valencia, E-mail: Regina.Moles@ific.uv.es The ATLAS experiment
More informationIntroduction. Bill Cooper LDC Meeting May 25,
The Vertex Detector in the SiD Concept Bill Cooper Fermilab (Layer 1) (Layer 5) VXD Introduction SiD is a closely integrated detector. Designs of the outer tracker and the vertex detector have been developed
More informationLHC Detector Upgrades
Su Dong SLAC Summer Institute Aug/2/2012 1 LHC is exceeding expectations in many ways Design lumi 1x10 34 Design pileup ~24 Rapid increase in luminosity Even more dramatic pileup challenge Z->µµ event
More informationOPERA: A First ντ Appearance Candidate
OPERA: A First ντ Appearance Candidate Björn Wonsak On behalf of the OPERA collaboration. 1 Overview The OPERA Experiment. ντ Candidate Background & Sensitivity Outlook & Conclusions 2/42 Overview The
More informationThe LiC Detector Toy program
The LiC Detector Toy program M Regler, W Mitaroff, M Valentan, R Frühwirth and R Höfler Austrian Academy of Sciences, Institute of High Energy Physics, A-1050 Vienna, Austria, EU E-mail: regler@hephy.oeaw.ac.at
More informationLHC-B. 60 silicon vertex detector elements. (strips not to scale) [cm] [cm] = 1265 strips
LHCb 97-020, TRAC November 25 1997 Comparison of analogue and binary read-out in the silicon strips vertex detector of LHCb. P. Koppenburg 1 Institut de Physique Nucleaire, Universite de Lausanne Abstract
More informationTiming properties of MCP-PMT
Photon Detector Workshop at Kobe, 27-29 June 27 Timing properties of MCP-PMT - Time resolution - Lifetime - Rate dependence K.Inami (Nagoya university, Japan) Introduction Photon device for TOP counter
More informationActivity on GEM by the Rome group since last meeting
OLYMPUS Collaboration DESY 24/Feb/21 Activity on GEM by the Rome group since last meeting Salvatore Frullani / INFN-Rome Sanità Group 1 Outline DESY test beam 9-2 December SBS Technical Review JLab 22
More informationAlignment of the ATLAS Inner Detector
Alignment of the ATLAS Inner Detector Heather M. Gray [1,2] on behalf of the ATLAS ID Alignment Group [1] California Institute of Technology [2] Columbia University The ATLAS Experiment tile calorimeter
More informationPhysics and Detector Simulations. Norman Graf (SLAC) 2nd ECFA/DESY Workshop September 24, 2000
Physics and Detector Simulations Norman Graf (SLAC) 2nd ECFA/DESY Workshop September 24, 2000 Simulation studies for a future Linear Collider We believe that the physics case for the LC has been made.
More informationTPC Detector Response Simulation and Track Reconstruction
TPC Detector Response Simulation and Track Reconstruction Physics goals at the Linear Collider drive the detector performance goals: charged particle track reconstruction resolution: δ reconstruction efficiency:
More information8.882 LHC Physics. Track Reconstruction and Fitting. [Lecture 8, March 2, 2009] Experimental Methods and Measurements
8.882 LHC Physics Experimental Methods and Measurements Track Reconstruction and Fitting [Lecture 8, March 2, 2009] Organizational Issues Due days for the documented analyses project 1 is due March 12
More informationAlignment and physics performance of the Belle II vertex detector
Alignment and physics performance of the Belle II vertex detector and T. Bilka et al. on behalf of the Belle II collaboration Charles University E-mail: jakub.kandra@karlov.mff.cuni.cz, bilka@ipnp.troja.mff.cuni.cz
More informationATLAS, CMS and LHCb Trigger systems for flavour physics
ATLAS, CMS and LHCb Trigger systems for flavour physics Università degli Studi di Bologna and INFN E-mail: guiducci@bo.infn.it The trigger systems of the LHC detectors play a crucial role in determining
More informationFull Simulation of Belle & Belle II SVD Detector (within ILC Framework)
Full Simulation of Belle & Belle II SVD Detector (within ILC Framework) Z. Drásal Charles University in Prague ILC Software Framework Summary Mokka: Geant 4 based, full simulation tool using a realistic
More informationSoLID GEM Detectors in US
SoLID GEM Detectors in US Kondo Gnanvo University of Virginia SoLID Collaboration Meeting @ JLab, 08/26/2016 Outline Design Optimization U-V strips readout design Large GEMs for PRad in Hall B Requirements
More informationStatus of the TORCH time-of-flight detector
Status of the TORCH time-of-flight detector Neville Harnew University of Oxford (On behalf of the TORCH collaboration : the Universities of Bath, Bristol and Oxford, CERN, and Photek) August 7-9, 2017
More informationALICE tracking system
ALICE tracking system Marian Ivanov, GSI Darmstadt, on behalf of the ALICE Collaboration Third International Workshop for Future Challenges in Tracking and Trigger Concepts 1 Outlook Detector description
More informationTopics for the TKR Software Review Tracy Usher, Leon Rochester
Topics for the TKR Software Review Tracy Usher, Leon Rochester Progress in reconstruction Reconstruction short-term plans Simulation Calibration issues Balloon-specific support Personnel and Schedule TKR
More informationOverview of SVT DAQ Upgrades. Per Hansson Ryan Herbst Benjamin Reese
Overview of SVT DAQ Upgrades Per Hansson Ryan Herbst Benjamin Reese 1 SVT DAQ Requirements and Constraints Basic requirements for the SVT DAQ Continuous readout of 23 040 channels Low noise (S/N>20 to
More informationThe CMS alignment challenge
The CMS alignment challenge M. Weber a for the CMS Collaboration a I. Physikalisches Institut B, RWTH Aachen, Germany Abstract The CMS tracking detectors are of unprecedented complexity: 66 million pixel
More informationSVT detector Electronics Status
SVT detector Electronics Status On behalf of the SVT community Mauro Citterio INFN Milano Overview: - SVT design status - F.E. chips - Electronic design - Hit rates and data volumes 1 SVT Design Detectors:
More informationTPC Detector Response Simulation and Track Reconstruction
TPC Detector Response Simulation and Track Reconstruction Physics goals at the Linear Collider drive the detector performance goals: charged particle track reconstruction resolution: δ reconstruction efficiency:
More informationElectron detector(s) decision to proceed with 2 detectors
Electron detector(s) decision to proceed with 2 detectors Direct hit detector (DH1K) reciprocal space Fast application (DH80K) real space imaging Thin nonlinear DEPFETs Thin (nonlinear) Fast DEPFETs Thin
More informationAlignment of the CMS silicon tracker using Millepede II
Journal of Physics: Conference Series Alignment of the CMS silicon tracker using Millepede II To cite this article: Peter Schleper et al 2008 J. Phys.: Conf. Ser. 119 032040 Related content - CMS silicon
More informationElectron and Photon Reconstruction and Identification with the ATLAS Detector
Electron and Photon Reconstruction and Identification with the ATLAS Detector IPRD10 S12 Calorimetry 7th-10th June 2010 Siena, Italy Marine Kuna (CPPM/IN2P3 Univ. de la Méditerranée) on behalf of the ATLAS
More informationThe Silicon Tracking System: Mechanical Integration and Alignement
EUDET The Silicon Tracking System: Mechanical Integration and Alignement SiLC Collaboration 12.12.2009 Abstract A brief review of the impact of some of the SiTRA-JRA2 related activities within the EUDET
More informationTracking and Vertexing performance in CMS
Vertex 2012, 16-21 September, Jeju, Korea Tracking and Vertexing performance in CMS Antonio Tropiano (Università and INFN, Firenze) on behalf of the CMS collaboration Outline Tracker description Track
More informationUpdate on PRad GEMs, Readout Electronics & DAQ
Update on PRad GEMs, Readout Electronics & DAQ Kondo Gnanvo University of Virginia, Charlottesville, VA Outline PRad GEMs update Upgrade of SRS electronics Integration into JLab DAQ system Cosmic tests
More informationSoLID GEM Detectors in US
SoLID GEM Detectors in US Kondo Gnanvo University of Virginia SoLID Collaboration Meeting @ JLab, 05/07/2016 Outline Overview of SoLID GEM Trackers Design Optimization Large Area GEMs for PRad in Hall
More informationStatus of the DCBA experiment
Status of the DCBA experiment 9 November, 2016 Hidekazu Kakuno Tokyo Metropolitan University International Workshop on Double Beta Decay and Underground Science, DBD16 Osaka University, JAPAN bb experiments
More informationValidation of the front-end electronics and firmware for LHCb vertex locator.
Validation of the front-end electronics and firmware for LHCb vertex locator. Antonio Fernández Prieto Universidade de santiago de compostela, Spain E-mail: antonio.fernandez.prieto@cern.ch Pablo Vázquez
More informationCMS Conference Report
Available on CMS information server CMS CR 2005/021 CMS Conference Report 29 Septemebr 2005 Track and Vertex Reconstruction with the CMS Detector at LHC S. Cucciarelli CERN, Geneva, Switzerland Abstract
More informationUpgrading the ATLAS Tile Calorimeter electronics
ITIM Upgrading the ATLAS Tile Calorimeter electronics Gabriel Popeneciu, on behalf of the ATLAS Tile Calorimeter System INCDTIM Cluj Napoca, Romania Gabriel Popeneciu PANIC 2014, Hamburg 26th August 2014
More informationVelo readout board RB3. Common L1 board (ROB)
Velo readout board RB3 Testing... Common L1 board (ROB) Specifying Federica Legger 10 February 2003 1 Summary LHCb Detectors Online (Trigger, DAQ) VELO (detector and Readout chain) L1 electronics for VELO
More informationEicRoot software framework
EicRoot software framework Alexander Kiselev EIC Software Meeting Jefferson Lab September,24 2015 Contents of the talk FairRoot software project EicRoot framework structure Typical EicRoot applications
More informationPrototyping of large structures for the Phase-II upgrade of the pixel detector of the ATLAS experiment
Prototyping of large structures for the Phase-II upgrade of the pixel detector of the ATLAS experiment Diego Alvarez Feito CERN EP-DT On Behalf of the ATLAS Collaboration 2017 IEEE NSS and MIC 26/10/2017
More information3D-Triplet Tracking for LHC and Future High Rate Experiments
3D-Triplet Tracking for LHC and Future High Rate Experiments André Schöning Physikalisches Institut, Universität Heidelberg Workshop on Intelligent Trackers WIT 2014 University of Pennsylvania May 14-16,
More informationSoLID GEM Detectors in US
SoLID GEM Detectors in US Kondo Gnanvo University of Virginia SoLID Collaboration Meeting @ Jlab, 01/13/2016 Outline Overview of SoLID GEM Trackers Large area GEM R&D @ UVa Update on APV25 Electronics
More informationTrack reconstruction of real cosmic muon events with CMS tracker detector
Track reconstruction of real cosmic muon events with CMS tracker detector Piergiulio Lenzi a, Chiara Genta a, Boris Mangano b a Università degli Studi di Firenze and Istituto Nazionale di Fisica Nucleare
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2008/100 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 02 December 2008 (v2, 03 December 2008)
More informationProgress in FDIRC & TOF
Progress in FDIRC & TOF J. Va vra, SLAC Content FDIRC prototype - Activities related to analysis of the last test beam run TOF detector - Summary of test results Next steps Appendix - PID electronics summary
More informationTracking and Vertex reconstruction at LHCb for Run II
Tracking and Vertex reconstruction at LHCb for Run II Hang Yin Central China Normal University On behalf of LHCb Collaboration The fifth Annual Conference on Large Hadron Collider Physics, Shanghai, China
More informationMuon Reconstruction and Identification in CMS
Muon Reconstruction and Identification in CMS Marcin Konecki Institute of Experimental Physics, University of Warsaw, Poland E-mail: marcin.konecki@gmail.com An event reconstruction at LHC is a challenging
More informationSimulation Study for EUDET Pixel Beam Telescope using ILC Software
Simulation Study for EUDET Pixel Beam Telescope using ILC Software Linear Collider Workshop, Hamburg, May/June 2007 Tatsiana Klimkovich DESY Tatsiana Klimkovich, Linear Collider Workshop, May/June 2007
More informationStudies of the KS and KL lifetimes and
Studies of the KS and KL lifetimes and BR(K ) with KLOE ± ± + Simona S. Bocchetta* on behalf of the KLOE Collaboration KAON09 Tsukuba June 9th 2009 * INFN and University of Roma Tre Outline DA NE and KLOE
More informationUsing only HyCal. Graph. Graph
Live charge weighted ep yield from all the 2GeV empty target runs Scattering angle from.7 to.9 deg, background dominated by upstream collimator (8%) Notice that here uncertainty from the live charge measurement
More information