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Forward Tagger Simulations Implementation in GEMC Moller Shield Tracking Studies R. De Vita INFN –Genova Forward Tagger Meeting, CLAS12 Workshop, June.

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Presentation on theme: "Forward Tagger Simulations Implementation in GEMC Moller Shield Tracking Studies R. De Vita INFN –Genova Forward Tagger Meeting, CLAS12 Workshop, June."— Presentation transcript:

1 Forward Tagger Simulations Implementation in GEMC Moller Shield Tracking Studies R. De Vita INFN –Genova Forward Tagger Meeting, CLAS12 Workshop, June 16th 2010

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3 GEANT4 Simulations The geometry of the Forward Tagger Calorimeter based on the PbW04 crystals has been implemented in GEMC 408 crystals 15x15x200 mm size Coverage from 1.8 to 5.2 deg. Tungsten beam pipe to shield from beam halo

4 GEANT4 Simulations Integration within the CLAS12 Geometry Completed and massive simulations of detector response in progress

5 GEANT4 Simulations Massive simulations of electromagnetic background to determine: 1)Rates 2)Radiation dose 3)Optimize Moeller shield in progress

6 Moeller Shield The shield consist of: a tungsten cone with inner opening angle of 0.75 degrees and outer opening angle of 2 degrees a carbon fiber structure which is part of the HTCC box vacuum inside the tungsten cone and within the cone and the carbon fiber structure The Moeller shield needs to optimized, varying the inner opening angle the length the distance from the target

7 Moeller Shield

8 Tracking Electron track reconstructed by tracking detectors located between the CD and the FT: Determine impact point on the calorimeter Reduce background by matching info from different detector systems Act as a veto for neutrals Sensitivity to particle momentum due to the  bend in the solenoid field Tracking planes location 1. Extend the forward tracking capability down to 2deg 2. Add a new plane in front of the calorimeter

9 Tracking Principle: electrons emitted at small angles are bent by the solenoid field the net effect is rotation in  of the track with negligible modifications of the polar angle the rotation is induced by the component of the solenoid field perpendicular to the tracks first tracking plane should be between 1 m from the target =3 deg electron track

10 Tracking 1) The size of the bend depends on the energy 0.5 GeV 1.0 GeV 1.5 GeV 2.0 GeV 2.5 GeV 3.0 GeV 3.5 GeV 4.0 GeV and only at small extend on the polar angle 2) The rotation of the electron plane occurs within the first meter from the solenoid center

11 Tracking This effect can be exploited to infer the electron momentum from the measured phi rotation For p> 500 MeV: one-to-one relation between momentum and phi rotation no significant dependence on the polar angle

12 Tracking First estimate based on GEANT simulations shows that % resolution on momentum and angles can be achieved with 2 tracking planes located in between the CD and FT calorimeter and spatial resolution of ~100um More details at http://clasweb.jlab.org/wiki/index.php/Tracking_studies

13 Work Plan Simulation and background studies: complete simulation of electromagnetic background to optimize the Moeller shield and determine the background rate and radiation dose on the FT Tracking: first simulation have proven the principle full simulation of realistic tracking system and reconstruction are needed


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