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AGATA S002 and S003 Coincidence Scans. Matthew Dimmock (mrd@ns.ph.liv.ac.uk). Overview. Issues with MGS Experimental versus MGS S002 versus S003 Ongoing work. Some issues with MGS. AGATA symmetric geometry. Passivation reduces surface currents. 2mm Isolant. No Isolant.
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AGATAS002 and S003 Coincidence Scans Matthew Dimmock (mrd@ns.ph.liv.ac.uk)
Overview • Issues with MGS • Experimental versus MGS • S002 versus S003 • Ongoing work
Some issues with MGS • AGATA symmetric geometry • Passivation reduces surface currents 2mm Isolant No Isolant
Some issues with MGS • Potential mapping • Back region where all charges are collected due to deformed potential surface 2mm Isolant No Isolant
Some issues with MGS • Electron drift velocity • Regions of unsaturated velocity 2mm Isolant No Isolant
Some issues with MGS • Electron drift – not a problem with calculations but consequence of model 2mm Isolant No Isolant r = 20mm = 290o z = 85mm r = 20mm = 290o z = 65mm
Some issues with MGS • “Charge sharing”
Test experimental alignment x C1 B3 D3 A3 E3 y F3 • Line 1 • T1 aligned • Good agreement Experimental centre contact pulses Experimental segment 15 (C3) & 33 (F3) pulses
Experimental versus MGS x C1 B3 D3 A3 E3 y F3 • Line 1 – real charge pulses MGS and experimental centre contact pulses MGS and experimental segment 15 (C3) & 33 (F3) pulses
Experimental versus MGS x C1 B3 D3 A3 E3 y F3 • Line 1 – Upper / Lower ICs Experimental and MGS segment C4 and F4 image charges Experimental and MGS segment C2 and F2 image charges
Experimental versus MGS x C1 B3 D3 A3 E3 y F3 • Vary MGS to fit experimental data 19mm Experimental and MGS segment F4 image charges 19mm Experimental and MGS segment F2 image charges Exp, z = 34mm MGS, z = 34mm Exp, z = 34mm MGS, z = 34mm
Experimental versus MGS x • Line 2, 7.5o clockwise B/C • T1 aligned • Good agreement C1 B3 D3 A3 E3 y F3 MGS and Experimental core pulses MGS and Experimental segment F3 (33) pulses
Experimental versus MGS x C1 B3 D3 • Line 1 – Upper / Lower ICs A3 E3 y F3 Segment E3 (Left) Image Charge Pulse Segment A3 (Right) Image Charge Pulses
Experimental versus MGS • Sum of squares difference for experimental and MGS data
Experimental versus MGS • Is sum of squares difference a result of poor time alignment
S002 Versus S003 • Quantify detector twist
Conclusions • MGS R5.02 is has been used to generate latest data • Two MGS data sets will be generated. The S003 set will factor in twist. • Basis sets have been partially generated to produce 3D chi squared difference to see where MGS fails • Bart and Benedikt code will be used to find best parameters.