Oct. 16, 1998Hobbs (thanks Hal)1 SMT Road Widths & Extra CFT Layers Current Situation Adding a 3rd CFT layer Using all 8 CFT layers Summary.

Slides:



Advertisements
Similar presentations
Impact parameter studies with early data from ATLAS
Advertisements

Proposal for a new design of LumiCal R. Ingbir, P. Ruzicka, V. Vrba October 07 Malá Skála.
Lyon Gantry Status TEC meeting Dec D. Contardo Module production in Lyon Rigidifier test on R4 Frame tolerance effect on assembly plates Short term.
1 Acceptance & Scraping Chris Rogers Analysis PC
1 Calice Analysis 02/03/09 David Ward ECAL alignment update David Ward  A few thoughts about ECAL alignment  And related issue of the drift velocity.
Jan. 2009Jinyuan Wu & Tiehui Liu, Visualization of FTK & Tiny Triplet Finder Jinyuan Wu and Tiehui Liu Fermilab January 2010.
Adding electronic noise and pedestals to the CALICE simulation LCWS 19 – 23 rd April Catherine Fry (working with D Bowerman) Imperial College London.
LHCb PatVeloTT Performance Adam Webber. Why Upgrade?  Currently we de-focus the beams o LHCb Luminosity ~ 2x10 32 cm -2 s -1 o ~ 1 interaction per bunch.
Rick Wilkinson New CSC Geometry u GEANT Simulation uses DDD Geometry è Uses active gas volumes u Digitization/Reconstruction adds a C++ geometry è Adds.
D. Peterson, “TPC Detector Response Simulation and Track Reconstruction”, Round Table, 23-Jan TPC Detector Response Simulation and Track Reconstruction.
Kin Yip MSU, Oct Efficiency-p t turn-on curve, offset & p t MC Simulation using UPG_GEANT with muons Study for the p t trigger thresholds in L1 (CFTTM)
1 G4MICE studies of PID transverse acceptance MICE video conference Rikard Sandström.
D. Peterson, “TPC Detector Response Simulation and Track Reconstruction”, LC-TPC-LBL, 18-Oct For example: TPC: 2.0 m O.R., 0.5 m I.R., 150  m spatial.
Measuring momentum at the TIF David Stuart, UC Santa Barbara June 25, 2007.
Chris Rogers, MICE CM16 Wednesday Plenary Progress in Cooling Channel Simulation.
WH  bb and WH  uu Studies Monica Dunford FTK Monthly Meeting March 13 th, 2007.
Tracking Efficiency and Momentum Resolution Analysis Chris Meyer UCSC ILC Simulation Reconstruction Meeting March 13, 2007.
October 20th, 2006 A. Mazzacane 1 4 th Concept Software First Results.
L1 CTT May 14, 2002 New Scheme for Tracking Marvin Johnson.
Silicon Tracking for Forward Electron Identification at CDF David Stuart, UC Santa Barbara Oct 30, 2002 David Stuart, UC Santa Barbara Oct 30, 2002.
Jean Favier OPERA Meeting Ankara 3/04/09 1 Some ECC features studied with GenIma Efficiency with no fog Efficiencies with fog Micro-track number versus.
1 N. Davidson Calibration with low energy single pions Tau Working Group Meeting 23 rd July 2007.
Chris Rogers, Analysis Parallel, MICE CM17 Progress in Cooling Channel Simulation.
1 Calice UK s/w meeting RHUL 24/1/06D.R. Ward David Ward Have previously reported on comparison of Feb’05 DESY data with Geant4 Monte Carlos. Issues with.
Since Rich wanted some relatively quick info on what detector might be needed to help MuTr pattern recognition, I did a scan on a central HIJING file I.
Status of the Beamline Simulation A.Somov Jefferson Lab Collaboration Meeting, May 11, 2010.
Error Analysis Significant Figures and Error Propagation.
IDAG Tracking Review  Groups have not yet submitted LOI  Avoid ‘temptation’ to regard as a Technical Design Review  Rules Specified –leave groups to.
LCWS 2004, ParisSonja Hillert, University of Oxfordp. 1 Flavour tagging performance analysis for vertex detectors LCWS 2004, Paris Sonja Hillert (Oxford)
Beam test results of Tile/fiber EM calorimeter and Simulator construction status 2005/03/05 Detector Niigata University ONO Hiroaki contents.
CALORIMETER system for the CBM detector Ivan Korolko (ITEP Moscow) CBM Collaboration meeting, October 2004.
Start Counter Collaboration Meeting September 2004 W. Boeglin FIU.
A Pattern Recognition Scheme for Large Curvature Circular Tracks and Its FPGA Implementation Example Using Hash Sorter Jinyuan Wu and Z. Shi Fermi National.
Muon-raying the ATLAS Detector
Vienna Fast Simulation LDT Munich, Germany, 17 March 2008 M. Regler, M. Valentan Demonstration and optimization studies by the Vienna Fast Simulation Tool.
Aerosol Limits for Target Tracking Ronald Petzoldt ARIES IFE Meeting, Madison, WI April 22-23, 2002.
Status of MAPS Geometry Simulation Yoshinari Mikami University of Birmingham 21 th April 2006 MAPS Meeting at Rutherford Appleton Laboratory.
LCWS 06 Bangalore, India, March Track fitting using weight matrix Nick Sinev, University of Oregon.
7 May 2009Paul Dauncey1 Tracker alignment issues Paul Dauncey.
Synopsis of Yang/Wang’s Analysis and Optimization on Single-Zone Binary Flat-Top Beam Shaper Blake Anderton Mon, Dec
Tilt angles reloaded, and status of some other things.
A Clustering Algorithm for LumiCal Halina Abramowicz, Ronen Ingbir, Sergey Kananov, Aharon Levy, Iftach Sadeh Tel Aviv University DESY Collaboration High.
1ECFA/Vienna 16/11/05D.R. Ward David Ward Compare these test beam data with Geant4 and Geant3 Monte Carlos. CALICE has tested an (incomplete) prototype.
Progress on the beam tracking instrumentation Position measurement device Tests performed and their resolution Decision on electronics Summary.
Start and Vertex Detector W. Boeglin, A.Klein Current Design: 3300 scintillating fibers 1mm diameter 3 double layers (1 axial, 2 stereo) cylindrical geometry.
Lukens - 1 Fermilab Seminar – July, 2011 Observation of the  b 0 Patrick T. Lukens Fermilab for the CDF Collaboration July 2011.
Sensitivity of HOM Frequency in the ESS Medium Beta Cavity Aaron Farricker.
CaTS and Dual Readout. CaTS – Calorimeter and Tracker Simulation Describe detector in gdml file (xml like) Define.
FNAL Beam test results A. Zhang, V. Bhopatkar, M. Phipps, J. Twigger, M. Hohlmann HEP Group A, Florida Tech 2013/11/18.
Vertex detector update 1 Oct Y. Sugimoto KEK.
1 Oct 2009Paul Dauncey1 Status of 2D efficiency study Paul Dauncey.
1 Hadronic calorimeter simulation S.Itoh, T.Takeshita ( Shinshu Univ.) GLC calorimeter group Contents - Comparison between Scintillator and Gas - Digital.
1 LumiCal Optimization Simulations Iftach Sadeh Tel Aviv University Collaboration High precision design May 6 th 2008.
Tracking Variable Study Follow up Ryan Kelley Boris Mangano Vivek Sharma.
Layer00 Efficiency Studies Stephen Levy, UChicago.
9th October 2003Danny Hindson, Oxford University1 Inner Detector Silicon Alignment Simple approach -Align in stages + rely on iteration Barrel to Barrel.
Alternative Code to Calculate NMH Sensitivity J. Brunner 16/10/
Eunil Won/Korea U1 A study of configuration for silicon based Intermediate Trackers (IT) July Eunil Won Korea University.
FP-CCD GLD VERTEX GROUP Presenting by Tadashi Nagamine Tohoku University ILC VTX Ringberg Castle, May 2006.
SHIP calorimeters at test beam I. KorolkoFebruary 2016.
DESY BT analysis - updates - S. Uozumi Dec-12 th 2011 ScECAL meeting.
Off-Detector Processing for Phase II Track Trigger Ulrich Heintz (Brown University) for U.H., M. Narain (Brown U) M. Johnson, R. Lipton (Fermilab) E. Hazen,
Ftksim at high luminosity Monthly meeting September 22, 2008 Anton Kapliy.
3/2/2000 Hobbs, Silicon Mtng 1 STT & SMT Assembly Precision Method Results –no in situ alignment –w/in situ alignment Conclusions Stress difference between.
Velocity of light in water
Simulation and Reconstruction code using Mathematica
Studies for Phase-II Muon Detector (|η| = ) – Plans
Slice Test: Preliminary Data Analysis The Ohio State University
Electron tagging possibilities with current data
Backgrounds using v7 Mask in 9 Si Layers at a Muon Higgs Factory
Presentation transcript:

Oct. 16, 1998Hobbs (thanks Hal)1 SMT Road Widths & Extra CFT Layers Current Situation Adding a 3rd CFT layer Using all 8 CFT layers Summary

Oct. 16, 1998Hobbs (thanks Hal)2 Current Method Use A, H layers of CFT –Require sensitivity for |b| < 0.2 cm |  | 1.5 GeV) –2 hits only: Road width driven by IP range, |b| < 0.2 cm Road width  2 mm (or  1 mm?) –D  Note 3363 (Uli) –Same width for all SMT layers

Oct. 16, 1998Hobbs (thanks Hal)3 See the following combinatoric scale

Oct. 16, 1998Hobbs (thanks Hal)4 And as a function of road width

Oct. 16, 1998Hobbs (thanks Hal)5 Add a 3 rd CFT Layer Vary track true b,  Find 3 fibers hit for b,  Bound road width –Try all 8 tracks touching edge of the 3 fibers (2 of 8 shown) –Only tracks meeting |b| and |  | constraints –Plot  at each SMT radius (circular approx OK) –Keep  MIN  MAX  TRUE for each layer Road:  *r A H

Oct. 16, 1998Hobbs (thanks Hal)6 Result: Road width vs. radius Plot is for NO |b|<0.2 mm constraint, with constraint, ROAD =  2mm

Oct. 16, 1998Hobbs (thanks Hal)7 Using all 8 CFT Doublets Choose true b, ,  0 (=0.0) Determine fibers hit Find widths for “all” tracks allowed by hit fibers (use random numbers) Plot width at each SMT layer

Oct. 16, 1998Hobbs (thanks Hal)8 One example (b=  =0) Lightly shaded area: w/constraint |b|<2 mm

Oct. 16, 1998Hobbs (thanks Hal)9 Conclusions... Adding only a 3 rd layer is little help –|b|<0.2cm still drives width Full information from 8 layers –Optimum road width, SMT layer dependent –Layer 4(outermost), Half width = 1 mm –Layer 1(innermost), Half width = 2 mm Impact of multiple scattering and CFT alignment precision unknown Make a few more sanity checks… –Fiber “resolution”: square w/width 1 mm –Simulate fiber bins? –Clear plot for 3 fiber case w/constraint