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Progress of CMOS CSA for Point Contact HPGe Detectors
Xuezhou Zhu, Zhi Deng* Department of Engineering Physics, Tsinghua University 04/10/2013 Symposium of the Sino-German GDT Cooperation Tubingen, Germany, 4/8~4/12, 2013
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Symposium of the Sino-German GDT Cooperation
Outlines Introduction Objectives What’s the noise limit of a CMOS CSA To what level it could be competing with JFET Methods Results and Discussion Summary 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Introduction ULE HPGe Detector for Dark Matter Search The key technologies for lowering the energy threshold is using small capacitance detector and ultra low noise readout Point-contact HPGe, ~1pF 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Objectives Noise components for CSA tm, ns As the detector capacitance goes down, the contribution from 1/f noise become non-dominant anymore! 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
What is the limit for 1/f noise Borrowed from Paul O’Connor’s talk in FEE2006 e.g., Kf = 10-25J, Cd=1pF ENCf ~ 5 e- Why not CMOS then? 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Methods Noise Optimization for 1pF Detectors Pulse reset PMOS for lower 1/f noise, with optimized size Adjustable bias current for noise study 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Circuit Design and Implementation 10ns rise time for negative signal for 200pF // 1kOhm load (A. Pullia and F. Zocca, 2009 IEEE NSS) 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Test Setup Shaper Power Supply Signal Generator Oscilloscope Bump Temperature sensor Vacuum chamber 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Mount with detector 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Results Electronics low temperature Cin=2pF 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Noise capacitor room temperature RC(ms) Noise ratio (tst, e/pF) 2 18.0 4 14.4 8 12.8 12 9.58 Very close to simulation results for small input capacitance, still some room to improve 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Detector leakage current Best Id : 1000mV*0.125pF/15.2ms = 8.25pA Typical Id : 80-120pA, very sensitive to detector mounting 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Veto fake signals by reset Using a wider version of reset signal to veto the fake signals 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Cs-137 Spectrum HV=230V, Id~100pA, RC=2ms 662keV peak 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Discussion Energy resolution: keV Fano limit: 1033 eV (F = 0.1) Electronics noise: 100pA leak current ~ 347 eV (50 e in rms) CMOS CSA ~ 174 eV (25 e in rms) 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Electronics noise when connected to the detector RC (ms) sV (mV) 0.5 33.3 1 20 2 10 4 6 13.3 12 The shaper gain is estimated to be 38 from the MCA address of 662keV peak. Hence the CSA noise is estimated to be: 206 e in rms or 1428 eV in FWHM But still… 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Peak Value Drift Peak area (cnts) Resolution (% FWHM) (eV FWHM) 550 0.39% 2582 1600 0.48% 3178 3600 0.597% 3952 1763 eV 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Non-Gaussian Distribution 2013/4/10 Symposium of the Sino-German GDT Cooperation
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Symposium of the Sino-German GDT Cooperation
Summary The noise performance of the CMOS CSA keeps improving, down to RC=12ms, Cd=2pF. But there is some room for shorter RC time, e.g. 2ms. The test with detector is very challenging and still far from the optimized conditions. Energy resolution of 0.4% to 0.68% for 662keV full-energy-peak can be achieved for short and long term measurements. 2013/4/10 Symposium of the Sino-German GDT Cooperation
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