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Status report Detector team
Dirk Weißhaar IKP Köln Acceptance test of three symmetric AGATA-detectors - energy resolution with standard analogue electronics - cross-talk with digital coincidence electronics (XIA) In-beam test: position resolution for Doppler correction - analysis is ongoing
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Questions: Fold dependent shift of add-back energies Negative and positive outliers (>0.5keV) of add-back energies
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Core signal is AC-coupled to segments via bulk capacity CsegX !
Split charge model HV Split charge Cseg1 Cseg2 Cc Core Seg1 Seg2 GΩ Core signal is AC-coupled to segments via bulk capacity CsegX ! Segment I sees Qind=Qcore*CsegI/(Cc+ΣCsegX)
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Standard Cc of AGATA
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For AGATA-detector bulk capacity of segments is ~1.3pF
→ 1.3pF/1246pF = 0.105% → shift 1.3MeV is ~1.4keV Notice: MINIBALL detector tested with Cc=5000pF should result in a shift of 0.15%. But measurement showed a shift of 0.54% (Cc=1200pf →0.59%).
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V1=Q1/Cf - Q2*C21/Cf2 Cross-talk, A. Pullia, Legnaro 2002 Cf C21
Seg1 Seg2 Cf pre1 pre2 C21 Q2 Q1 V1=Q1/Cf - Q2*C21/Cf2 Cf=1pF → C21=1fF yields to 0.1% crosstalk Eγ=E1+E2, a=C21/Cf, b=C12/Cf Emeasured=Eγ – aEγ - (b-a) E1 shift tilt Always Emeasured ≤ Eγ
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AGATA cold preamplifier
16mm
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Crosstalk E1 → E2
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Measurement of the tilt by unfolding 2-fold spectra
in spectra Eγseg1> Eγseg2 and Eγseg2 >Eγseg1
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Position of cold preamps for nearest neighbours event
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Nevertheless: cross-talk <10-3
Conclusion for cross-talk Split charge model solves the fold dependent energy shift of the add-back spectra. Preamplifier cross–talk yields a negative shift and a tilt for the add-back energies. No systematics has been found for the outliers in the add-back spectra for the three detectors (same cryostat, same cold and warm preamplifiers) Model for positive outliers? Nevertheless: cross-talk <10-3
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~ 15% of core peak intensity
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The ‘bow’-effect only occurs in
nearest neighbour add-back of front segments The ‘bow’-effect not occurs in any other 2-fold combination (also between not neighbouring front segments !)
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