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UTA GEM DHCAL SIM

UTA GEM DHCAL SIM. Introduction Digital Hadron Calorimeter Requirements GEM in the sensitive gap UTA GEM DHCAL Prototype Status Simulation Status Summary. J. Yu* Univ. of Texas at Arlington Nov. 7 - 9, 2002 NIU/NICADD.

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UTA GEM DHCAL SIM

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  1. UTA GEM DHCAL SIM • Introduction • Digital Hadron Calorimeter Requirements • GEM in the sensitive gap • UTA GEM DHCAL Prototype Status • Simulation Status • Summary J. Yu* Univ. of Texas at Arlington Nov. 7 - 9, 2002 NIU/NICADD (*On behalf of the UTA team; A. Brandt, K. De, S. Habib, V. Kaushik, J. Li, M. Sosebee, A. White)

  2. Introduction • LC physics topics • Distinguish W from Z in two jet final states  Good jet mass resolution • Higher Jet energy resolution; • Excellent jet angular resolution • Energy flow algorithm is one of the solutions • Replace charged track energy with momentum measured in the tracking system • Requires efficient removal of associated energy cluster  Good position resolution • Higher calorimeter granularity • Use calorimeter only for neutral particle energies • Best known method for jet energy resolution improvement • Large number of readout channel will drive up the cost for analogue style energy measurement  Digital HCAL • Tracking calorimeter with high gain sensitive gap Jae Yu: GEM Based DHCAL

  3. Goals for UTA DHCAL Development • Develop digital hadron calorimetry for use with EFA • Aim for cost effectiveness and high granularity • Look for a good tracking device for the sensitive gap • Develop GEM cell(s) and prototype • Develop module/stack design for EFA optimization • Simulate GEM behavior in calorimeter • Implement GEM readout structure into simulation • Develop EF and calorimeter tracking algorithms • Cost effective, large scale GEM DHCAL Jae Yu: GEM Based DHCAL

  4. Why GEM? • GEM developed by F. Sauli (CERN) for use as pre-amplification stage for MSGC’s • Allow flexible and geometrical design, using printed circuit readout  Can be as fine a readout as GEM tracking chamber!! • High gains, above 104,with spark probabilities per incident  less than 10-10 • Fast response • 40ns drift time for 3mm gap with ArCO2 • Relatively low HV • A few 100V per each GEM gap compared to 10-16kV for RPC • Rather reasonable cost • Foils are basically copper-clad kapton • ~$400 for a specially prepared and framed 10cmx10cm foil Jae Yu: GEM Based DHCAL

  5. Large amplification 140mm 70mm CERN-open-2000-344, A. Sharma Jae Yu: GEM Based DHCAL

  6. GEM gains High gain Low voltage differential!! CERN GDD group Jae Yu: GEM Based DHCAL

  7. Double GEM DHCAL Design Anode pad Embeded onboard readout Ground Thr. Thr. AMP DISC AMP DISC REG REG Ground to avoid cross-talk Digital/serial output Preliminary readout design Jae Yu: GEM Based DHCAL

  8. Double GEM test chamber • Sufficient space for foil manipulation • Readout feed-through, retaining large space for ease of connection • Clear cover to allow easy monitoring • Readout pads connection at the top 2cmx2cm pad design J. Li, UTA Jae Yu: GEM Based DHCAL

  9. UTA GEM Test Chamber HV layout Drift gap HV fed from one supply but individually adjusted  Good to prevent HV damage on the foils 2.1kV Transfer gap Induction gap Jae Yu: GEM Based DHCAL

  10. UTA GEM Prototype Status • Readout circuit board (2cmx2cm pads) constructed • HV Connection implemented • Two GEM foils in the UTA Nano fabrication facility cleanroom • Preamp in hand and characterization completed (LeCroy HQV800) Amplification factor of 300 for 5xGEM size signal (LeCroy HQV800 ) Jae Yu: GEM Based DHCAL

  11. Want to know how GEM Foils look like? Jae Yu: GEM Based DHCAL

  12. Single GEM gain/discharge probability • Simulation study in progress using single pions before multi-jets • Determine Maximum total charge deposit in a cell of various sizes and gains • Study fake signal from spiraling charged particle in the gap A.Bressan et al, NIM A424, 321 (1998) Jae Yu: GEM Based DHCAL

  13. UTA Simulation Status • Two masters students have been working on this project • Pandora-Phythia implementation and HEPEvt ASCII output in place • Mokka successfully installed • Mokka Geometry database downloaded and installed at UTA • Completed single pion studies using default geometry • Reproduced expected response • Energy resolution seems to be reasonable also • Preliminary mixture GEM geometry implemented • Single pion study with mixture GEM begun • Root macro and JAS based analysis packages developed • Proceed with more detailed GEM geometry implementation Jae Yu: GEM Based DHCAL

  14. Single Pion Studies w/ Default TESLA Geometry • Single pion events using Mokka particle gun command. • Incident energy range: 5 – 200GeV • kinematics information on primary particles in the files • Developed an analysis program to read total energies deposited per pion for each incident energy. • Mean Energy vs Incident pion energies • Energy conversion from the slope of the straight line • Conversion factor is 3.47% and agrees with the computed sampling fraction Jae Yu: GEM Based DHCAL

  15. TESLA TDR Geometry • Ecal – Electromagnetic Calorimeter Material: W/G10/Si/G10 plates (in yellow) • 1mm W absorber plates • 0.5 mm thick Si, embeded 2 G10 plates of 0.8 mm each • Hcal – Hadronic Calorimeter • Material: • 18 mm of Fe • 6.5 mm of Polystyrene scintillator (in green) Jae Yu: GEM Based DHCAL

  16. TESLA TDR detector live energy deposit for single pions Jae Yu: GEM Based DHCAL

  17. TESLA TDR Elive vs Ep % Jae Yu: GEM Based DHCAL

  18. TESLA TDR CAL Single Pion Resolution Jae Yu: GEM Based DHCAL

  19. GEM Simulation Status • Mokka Geometry database downloaded and installed at UTA • New Geometry driver written  Mixture GEM geometry implemented Need to use ArCO2 only • Single pion study begun for discharge probability • Initial study shows that the number of electron, ion pair with gain of 104 will be on the order of 107 for single 200GeV pions • Getting pretty close to the 108 from other studies  Might get worse for jets from W pairs, due to fluctuation • Need more studies to compute the discharge probability. • Cell energy deposit being investigated to determine optimal threshold based on cell energy  Proceed to energy resolution studies • Determine optimal gain using live energy deposit vs incident energy Jae Yu: GEM Based DHCAL

  20. GEM Prototype Geometry Jae Yu: GEM Based DHCAL

  21. Venkat, TSAPS Meet Oct 10 - 12, 2002 GEM Geometry Implementation Mechanics in Mokka • TDR / Hcal02 Model chosen for modification • Fe-GEM sub-detector instead of the existing Fe-Scintillator • New driver for the HCal02 sub-detector module • Local database connectivity for HCal02  Database downloaded and implemented at UTA Courtesy: Paulo deFrietas Jae Yu: GEM Based DHCAL

  22. Single Pion Cell Energy Deposit in GEM HCal Jae Yu: GEM Based DHCAL

  23. Single pion Energy with GEM 50GeV p ELive 15GeV p EMeas 10.6MeV Jae Yu: GEM Based DHCAL

  24. GEM Sampling Weight Sampling: 2~4x10-3 Statistics too low to produce reliable gaussian fit  This depends heavily on EM section without proper GEM gain factor taken into account. Jae Yu: GEM Based DHCAL

  25. Summary • Hardware prototype making significant progress • GEM foils delivered and are in the clean room for safe keeping • Preamp and Discriminator in hands  Preamp characterized • HV System implemented • Readout Pad implemented • Almost ready to put GEM foils in the prototype box • GEM foil mass production being looked into by 3M in Austin, Texas • Simulation effort made a marked progress • Single pion study of Mokka default TESLA TDR geometry complete • Analysis tools in place and seem to work well • The resolution seems to be reasonable • Preliminary GEM Mixture geometry implemented • Need to redo the response study with gain factored in… • Initial estimate of e+Ion pair seems to be at about 107 for 200GeV pions • Local Geometry database implemented • Optimal threshold for digitization and gain factor will come soon • Will soon move onto realistic events, WW, ZZ, or t`t  jets • Still ways to go before effective EFA and TRKA studies Jae Yu: GEM Based DHCAL

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