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Status of the muon simulations

Status of the muon simulations. Anna Kiseleva. Outline. Simulation environment Muon software geometry of the muon system (MuCh) segmentation of the muon detector layers clustering Muon tracking Results of the reconstruction Simulation activities in India FLUKA calculations Next steps.

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Status of the muon simulations

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  1. Status of the muon simulations Anna Kiseleva

  2. Outline • Simulation environment • Muon software • geometry of the muon system (MuCh) • segmentation of the muon detector layers • clustering • Muon tracking • Results of the reconstruction • Simulation activities in India • FLUKA calculations • Next steps

  3. Simulation environment • trunk (release Jun 09) of the cbmroot • background – central UrQMD at 25 AGeV • signal: ω • detector setup • muon magnet and muon field • pipe shielding • STS (standard) • MuCh (simple and modular design)

  4. Detector system 20 20 20 30 35 100 cm STS 30 cm Total size: 405 cm total size of MuCh in release Apr 08 ~ 327 cm

  5. Muon software: geometries and hit producer • Evgeny Kryshen (PNPI) • Mikhail Ryzhinskiy (PNPI & SPbSPU) • Alexander Zinchenko (JINR) • Test of software – Anna Kiseleva (U. Frankfurt)

  6. Geometries of the MuCh simple design modular design modular design with straw tubes

  7. Modular design of MuCh • Dead zones → missing hits • Overlaps → double hits

  8. Automatic segmentation // Number of stations seg->SetNStations(6); // Set minimum allowed resolution for each station Double_t sigmaXmin[] = {0.08, 0.08, 0.08, 0.08, 0.08, 0.08}; Double_t sigmaYmin[] = {0.08, 0.08, 0.08, 0.08, 0.08, 0.08}; seg->SetSigmaMin(sigmaXmin, sigmaYmin); // Set maximum allowed resolution for each station Double_t sigmaXmax[] = {0.6, 0.6, 0.6, 0.6, 0.8, 1.}; Double_t sigmaYmax[] = {0.6, 0.6, 0.6, 0.6, 0.8, 1.}; seg->SetSigmaMax(sigmaXmax, sigmaYmax); // Set maximum occupancy for each station Double_t occupancyMax[] = {0.05, 0.05, 0.05, 0.05, 0.05, 0.05}; seg->SetOccupancyMax(occupancyMax);

  9. Manual segmentation # General informationNumber of stations : 6# Station specificationNumber of channels : 128 128 128 128 128 128Number of regions : 4 4 3 3 3 3# Station 1Region radii [cm] : 19.6 30.8 47.6 70Pad width [cm] : 0.28 0.56 1.12 2.24Pad length [cm] : 0.28 0.56 1.12 2.24# Station 2Region radii [cm] : 26.6 41.8 64.6 96Pad width [cm] : 0.56 1.12 2.24 4.48Pad length [cm] : 0.56 1.12 2.24 4.48# Station 3Region radii [cm] : 33.6 52.8 120Pad width [cm] : 1.12 2.24 4.48 Pad length [cm] : 1.12 2.24 4.48 # Station 4Region radii [cm] : 42 66 150Pad width [cm] : 1.12 2.24 4.48Pad length [cm] : 1.12 2.24 4.48# Station 5Region radii [cm] : 51.1 80.3 182.5Pad width [cm] : 1.12 2.24 4.48Pad length [cm] : 1.12 2.24 4.48# Station 6Region radii [cm] : 69.3 108.9 247.5Pad width [cm] : 1.12 2.24 4.48Pad length [cm] : 1.12 2.24 4.48

  10. Segmentationfor simple design of MuCh ~ 390 000 channels

  11. Segmentationfor modular design of MuCh ~ 560 000 channels

  12. Muon Tracking • Andrey Lebedev (GSI, LIT JINR) • Test of the tracking – Anna Kiseleva (U. Frankfurt)

  13. μJ/ψ μω Muon tracking J/ψ→μ+μ– ρ0→μ+μ– J/ψ→μ+μ– ω→μ+μ– φ→μ+μ– ω→μ+μ–

  14. Algorithm of the muon tracking • Tracking is based on • Track following • Kalman Filter (KF) • Different hit-to-track association techniques (nearest neighbor, branching, weighting) • Two main steps: • track finding • track selection

  15. Global tracking TOF TRD MUCH STS Hit-to-track merging Global tracking L1 STS tracking STS tracking Global Tracking + TOF hit to track merging

  16. Tracking performance Andrey Lebedev Events 1000 UrQMD at 25 AGeV + 10 mu in each event all muons Branching tracking Efficiency in %

  17. Results of the full reconstruction ω→μ+μ- + central Au+Au collisions at 25 AGeV • Cuts: • χ2prim.vertex < 2.5 • ≤ 4 STS hits • χ2MuCh < 40 • ≥ 15 MuCh hits • Cuts: • χ2prim.vertex < 2 • ≤ 4 STS hits • χ2MuCh < 42.5 • ≥ 14 MuCh hits

  18. Invariant mass spectrum ω→μ+μ- + central Au+Au collisions at 25 AGeV modular design simple design

  19. Clustering CbmMuchDigitizeAdvancedGem* digitize = new CbmMuchDigitizeAdvancedGem("MuchDigitizeAdvancedGem", digiFile, iVerbose); digitize->SetSpotRadius(0.15); digitize->SetQThreshold(3); digitize->SetQMaximum(500000);digitize->SetNADCChannels(256);

  20. Clustering CbmMuchFindHitsAdvancedGem* findHits = new CbmMuchFindHitsAdvancedGem("MuchFindHitsAdvancedGem", digiFile, iVerbose); Produces hits in GEM-like modules using different clustering algorithms. Clustering algorithms can be chosen by the switch SetAlgorithm(Int_t iAlgorithm) Several clustering algorithms are supported 0 – Simple with threshold=0 1 – Simple 2 – Ward (fuzzy clustering) 3 – Simple + Ward 4 – Divisive clustering 5 – Simple + divisive clustering The Default value is 1: Simple Clustering Algorithm // --- Set Algorithm for clustering findHits->SetAlgorithm(1); Divisive Clustering Method

  21. Event display

  22. Results of the full reconstruction with clustering ω→μ+μ- + central Au+Au collisions at 25 AGeV • Cuts: • χ2prim.vertex < 2 • ≤ 4 STS hits • χ2MuCh < 42.5 • ≥ 14 MuCh hits modular design of MuCh

  23. Invariant mass spectrum ω→μ+μ- + central Au+Au collisions at 25 AGeV without clusters with clusters

  24. Activities in India Students working on various topics.. • Partha(VECC), Hemen (GU) : Trigger, SIS100, physics simulation • Bipasha (CU): dynamic range simulation, J/Psi physics at FAIR • Arun: Geometry study • Manish, Irshad (Jammu U) EVO meet every Thursday: co-ordinator: Z. Ahammed

  25. Trigger simulations • Partha Pratim Bhaduri (VECC, India)

  26. Take 3 hits from the trigger station with one from each of the 3 layers & fit with st. line both in X-Z & Y-Z plane passing through the origin (0. 0) i.e. X = m0*Z ; Y=m1*Z Make all possible combinations Find χ2 & apply cut on both χ2X & χ2y Hit combination satisfying the cuts is called a triplet. Hits once used for formation of a triplet is not used further. Find m0 & m1 of the fitted st. lines Define a parameter α=√(m02+m12) Apply cut on α Trigger station (0,0,0) Magnetic field Trigger algorithm

  27. Results • Input: • background – 80 000 minimum bias events at 25 AGeV Au+Au collisions • signal – J/ψ→μ+μ- in 1000 minimum bias events

  28. Future plans • Prepare a look-up table for different values of cut parameters & corresponding values of background suppression factor & signal reconstruction efficiency. • Implementation of TRD in the present scheme. • Study pad resolution effect. • Formation of CbmMuchTrigger class to be run in chain.

  29. Study of Manual Segmentation of MuCh • Arun Prakash (High Energy Physics Lab Department of Physics Banaras Hindu University Varanasi-221005)

  30. Different segmentation schemes

  31. Efficiency of the reconstructed muons from J/ψ

  32. Future plans • To look into other parameters like invariant mass, acceptance plot, momentum distribution etc. • Add clustering • Study auto-segmentation

  33. SIS-100 simulation • Charm simulations for SIS100 energies using HSD generator • Optimization of the muon geometry (N of stations/pad-sizes) • Arun (and Dr. Viyogi) will be at GSI working on this

  34. FLUKA calculations • Anna Kiseleva (U. Frankfurt)

  35. Radiation dose simulations (Denis Bertini) 13. CBM Collaboration MeetingMarch 9-13, 2009, GSI Darmstadt

  36. Compact MuCh scoring planes target 20 20 20 30 40 cm • Absorber • material: • Fe • C • W

  37. UrQMD events central mBias

  38. mBias UrQMD original UrQMD UrQMD with rotated reaction plane

  39. Next steps • Muon system optimization: number of detector layers and thickness of the absorbers • Optimization of the segmentation scheme • Implementation of the realistic detector parameters from the beam test • Radiation dose calculation with FLUKA for all detector systems

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