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Status of the Tagger Hall Background Simulation Simulation A. Somov, Jefferson Lab Hall-D Collaboration Meeting, University of Regina September 9 2010
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Analysis Overview Update Tagger Hall Geant geometry - narrow dipole magnet (new magnetic field map) - smaller vacuum chamber ( ~ 1.5 m shorter ) - new position of the focal plane and detectors - realistic geometry for the electron beam dump Study neutron background at the detector plane ( SiPM radiation hardness ) - use Radiation Control Geant 3.21 simulation provided by Pavel Degtyarenko - compare neutron doses with FLUKA Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 2
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Tagger Hall and Beam Dump Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 3 Z (cm) X (cm) Goniometer Quadrupole Magnet Dipole Magnet Vacuum Chamber Labyrinth Wall 1 Lab Wall 2 Lab Wall 3 Beam Dump e - Beam photons Detector plane Deflection angle for 12 GeV electrons: 13.4 Magnet rotation: 6.5 Focal plane angle: 8.05
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Tagger Hall Geometry Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 4 Possible sources of background: Flange of the vacuum chamber Electron beam pipe Flange Electron pipe Z (cm) X (cm) Dipole magnet cross-section (X-Y plane) 3 cm gap 12GeV electrons Z (cm) X (cm) 2630.1-475.8 2649.7-480.4 2785.8-512.9 Position of 12 GeV electrons at beam monitors: Magnet poles
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Downstream end of Vacuum Chamber & Electron Pipe Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 5 Z (cm) X (cm) Detector plane 9 GeV electrons 12 GeV electrons Vacuum Chamber Rectangular Beam Pipe 1 + 3 = 4 wide Flange End of exit window
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Simulation Overview Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 6 Estimated neutron background originating in the Tagger Hall and the beam dump enclosure. Particles were ‘stopped’ before the dump, more CPU is needed ( high-luminosity corresponds to ~10 13 electrons/sec; 1 event – 0.4 sec) - determine neutron flux and energy spectrum of neutrons at the focal plane: L = 852 cm, h = 100 cm - use biological damage conversion curve to estimate neutron dose Note: To estimate radiation damage, we have to use effective damage curve of Si (to be done). The neutron energy spectrum looks ‘similar’ to that used by Yi in his studies can use his numbers to estimate the dark rate increase Study background for 2 widths of the electron pipe: 3 and 6 between full energy electrons and the pipe walls
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Origin of Neutrons Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 7 Z (cm) X (cm) Vacuum chamber flange Electron Pipe Tagger Hall walls Magnet poles Air
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Neutron Energy Spectrum at the Detector Plane Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 8 Neutron kinetic energy ( MeV ) Biological damage coefficients Neutron energy spectrum pSv cm 2
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Neutron Dose Estimates (preliminary) Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 2 Z (cm) Events Neutron distribution along the focal plane 3 pipe: 0.6 rem/hour 6 pipe: 0.46 rem/hour Microscope counters region: 0.2 rem/hour According to Yi ’ s studies the dark current increases by a factor of 5 for the accumulated dose of 60 rem Further studies/geometry optimization is neede – work in progress
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Further Plans Status of the Tagger Hall Background Simulation, Hall-D Collaboration Meeting, September 9 2010 2 The first studies indicate large neutron background at the detector plane We have to check Geant geometry and ‘ optimize ’ layouts of the electron beam pipe and the downstream flange of the vacuum chamber - use a window or low density material for the beam pipe wall … Check Pavel Degtyarenko ’ s Geant with FLUKA (work in progress) We need to develop a plan to use other detectors instead of SiPM ’ s if the neutron background appears to be really high ….
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