HV Power Supply Filtering and EMI to Readout Sergio Rescia and Bo Yu Brookhaven National Laboratory Sept. 18, 2018
HV Supply Filter 2 x 100 MW 95 p. F 2 x 100 MW 1000 p. F 95 p. F 230 p. F
HV Supply Filter 3. 9 n. F
Heinzinger PNChp 300000 -1 neg Vripple=1. 8 V fripple=100 Hz + 30 k. Hz switching frequency
HV Filter + PA+Shaper Equivalent Circuit
Signal (LARASIC PA/Shaper, High Gain) Qinj=1 f. C (6000 e-) Vpeak=25 m. V (high Gain: 25 m. V/f. C) Noise= 600 e-rms (2. 5 m. Vrms)
HV Ripple= 1. 8 V (10 ppm of HVnom=180 k. V)
HV Ripple at output HV Ripple < 0. 5 m. V PP < 0. 15% LSB <0. 02% random noise rms
Ripple on Cathode Plane VEMI, cathode=260 m. V PP
HV Filter Attenuation f=100 Hz ATT=-74 d. B (1/5000) f=30 k. Hz ATT=-134 d. B (1/5 E 6)
Switching Frequency EMI (30 k. Hz)
2 nd Order Effects (EMI Crosstalk) NOT PERFECT Virtual Ground
EMI Crosstalk VEMICT<10 n. V PP < 2% direct EMI
Conclusion • HV Filter very effective (ATT~1/5000 at 100 Hz) • Direct EMI to a U wire preamplifier <0. 5 m. V PP (0. 15% of LSB) (@ gain 25 m. V/f. C) • 2 nd Order Effects (EMI “Crosstalk”) <2% of direct crosstalk • Good filtering of grid plane important to avoid 2 nd order crosstalk
Additional Slides
Dune HV Ripple model used for calculations on HV Filtering HV RIPPLE HV FILTER K-A+GRID PREAMP HV RIPPLE • • Tpeak=1μs Gain=25 m. V/p. C AC coupling: 1 ms RHV=100 MΩ or 200 MΩ AC COUPLING