1 / 18

E-Flow Optimization of the HCAL for a LC Detector – ANL Status Report

E-Flow Optimization of the HCAL for a LC Detector – ANL Status Report. S. Magill , A. Bamberger*, S. Chekanov, G. Drake, S. Kuhlmann, B. Musgrave, J. Proudfoot, J. Repond, R. Stanek, R. Yoshida Argonne National Laboratory. ANL R&D Goals E-flow Optimization Progress RPC Readout R&D

atalo
Download Presentation

E-Flow Optimization of the HCAL for a LC Detector – ANL Status Report

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. E-Flow Optimization of the HCAL for a LC Detector – ANL Status Report S. Magill, A. Bamberger*, S. Chekanov, G. Drake, S. Kuhlmann, B. Musgrave, J. Proudfoot, J. Repond, R. Stanek, R. Yoshida Argonne National Laboratory • ANL R&D Goals • E-flow Optimization Progress • RPC Readout R&D • Summary * Permanent address – Freiburg University

  2. LC HCAL R&D Goals at ANL - Motivation Physics Requirement : separate W, Z using dijet mass in hadronic decay mode (~70% BR) Detector Goal : measure jets with energy resolution /E ~ 30%/E • Optimize HCAL to be used with ECAL and Tracker in E-flow jet reconstruction – • Charged particles ~ 60% of jet energy -> Tracker • Photons ~ 25% of jet energy -> ECAL • Neutral Hadrons ~ 15% of jet energy -> HCAL Calorimeter challenge : charged/neutral shower separation requires high granularity, both transverse and longitudinal, to reconstruct showers in 3-D

  3. LC HCAL R&D Goals at ANL – Scope of Work • Optimize, in simulation, the design for an HCAL which, when used in an E-flow jet reconstruction algorithm, can reconstruct jets with /E ~ 30%/E. • study absorber type/thickness with JAS, standalone GEANT3 program • tune transverse granularity and longitudinal segmentation in JAS • test both analog and digital readout techniques • optimize E-flow algorithm • Investigate the feasibility of using Resistive Plate Chambers (RPCs) as the active media in the HCAL. • avalanche vs streamer mode • noise reduction, signal optimization, readout schemes • Develop electronics readout schemes for the optimized HCAL. • digital vs multi-threshold analog • efficient data compression

  4. Towards HCAL Optimization   Jet E Resolution (% x E)  Digital Analog Readout Log10 Cell Size (cm2) • How we will optimize HCAL : • Cell size determination • Separation of charged/neutral clusters in 3-D • Cluster algorithms • E-weighted cell association to clusters (analog readout) • Tracking clusterer (digital readout) • Fine tuning of absorber type density : W/Pb/U vs SS/Cu and thickness

  5. Java Analysis Studio (JAS) e+e- ZZ (500 GeV CM) • SD Detector : • ECAL • 30 layers • W(0.25 cm)/Si(0.04 cm) • ~20 X0, 0.8 I • ~5 mm X 5 mm cells • HCAL • 34 layers • SS(2.0 cm)/Scin(1.0 cm) • ~40 X0, 4 I • ~1 cm X 1 cm cells • Modified SD A: • ECAL • 30 layers • W(0.25 cm)/Si(0.04 cm) • ~20 X0, 0.8 I • ~1 cm X 1 cm cells • HCAL • 60 layers • W(0.7 cm)/Scin(1.0 cm) • ~120 X0, 4.5 I • ~1 cm X 1 cm cells • Modified SD B: • ECAL • 30 layers • W(0.25 cm)/Si(0.04 cm) • ~20 X0, 0.8 I • ~1 cm X 1 cm cells • HCAL • 60 layers • W(0.7 cm)/Scin(1.0 cm) • ~120 X0, 4.5 I • ~3 cm X 3 cm cells Soon to come – 5 cm X 5 cm HCAL cells -> ECFA/DESY HCAL

  6. JAS Example – Neutral Particles in CAL • Charged particles in tracker • Neutral particles in CAL • -  in ECAL • - KL0, n, nbar in HCAL

  7. Photon Analysis Analog Readout /mean ~ 15% Analog Readout – perfect Gamma cluster

  8. Photon Analysis Digital Readout non-linear behavior for dense showers /mean ~ 24% Digital Readout – perfect cluster Digital worse than analog readout

  9. KL0 Analysis – SD Detector Analog Readout /mean ~ 30% Compare to digital 

  10. linear behavior for hadron showers KL0 Analysis – SD Detector Digital Readout /mean ~ 26% Average : ~43 MeV/hit Analog EM + Digital HAD x calibration

  11. KL0 Analysis – Modified SD • Analog Readout SD B (3 cm X 3 cm) SD A (1 cm X 1 cm) /mean ~ 35% /mean ~ 26%

  12. KL0 Analysis – Modified SD • Digital Readout SD B (3 cm X 3 cm) SD A (1 cm X 1 cm) /mean ~ 25% /mean ~ 20%

  13. HCAL (only) Digital Results SD B SD 1 cm X 1 cm /mean ~ 28% SD A /mean ~ 32% 3 cm X 3 cm /mean ~ 28% 1 cm X 1 cm

  14. E-Flow Algorithm Systematic Approach : Tracks first (60%), Photons next (25%), Neutral hadrons last (15%) • 1st step -Track extrapolation thru Cal – substitute for Cal cells in road (core + tuned outlyers) – Cal granularity optimized for separation of charged/neutral clusters • 2nd step - Photon finder (use shower shape info) • 3rd step -Neutral hadron clusterer • 4th step –Jet Algorithm on E-flow objects • or • 3rd step -Jet Algorithm on Tracks and Photons • 4th step –include remaining Cal cells in jet (cone?)

  15. RPC Readout Development         • Using RPC from FNAL (P. Mazur) : • size: 25 x 25 cm2 • gas gap 2 mm • glass plates 2 mm thickness • resistive electrodes 40 kOhm/square • pad readout behind the anode electrode • gas: Ar 30% Isob. 8% Freon 62% (a la BELLE) • pad structure of 4x4 cm2, 2x2 cm2, 1x1cm2 • coupled to to give configurations • all pads + frame • all pads • 5(4x4)+2(2x2) cm2  • 4x4+2(2x2) cm2  

  16. Chamber Operation • avalanche mode observed for HV < 8.2 kV, few pC charge • change to streamer mode HV > 8.5 kV few 100pC • streamer mode has multiple streamers as HV increases, charge of a streamer is a slow function of the HV • streamers are seperated in time, but merge at HV > 9.2 kV • efficiency > 95% • single rate compatible with cosmics

  17. Readout of pads • size of the pad is varied for finding the spatial extension of the induced charge • effective size has a radius of about 6 cm • known to depend on the resistivity of the HV electrodes, here: 40 kOhm/square • measure charge of streamers for events at readout pad, compare with those taken at a distance of ~ 6 cm Cross talk (intergration time here: 100 ns) Next steps : higher resistivity of electrodes reduces lateral coupling of the pads.

  18. Summary • Starting studies of HCAL optimization for E-Flow jet analysis • optimal transverse cell size and longitudinal segmentation • optimal absorber material/thickness • analog vs digital readout • Starting development of E-Flow analysis tools • cluster algorithms for analog/digital modes • separation algorithms for clusters • Studying characteristics of RPC readout for HCAL

More Related