a latchup topology to investigate novel particle detectors
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A latchup topology to investigate novel particle detectors Alessandro Gabrielli a , Mauro Lolli a , Giulio Villani b , Danilo Demarchi c , Antonio Ranieri d a I.N.F.N. and Physics Department University of Bologna b STFC Rutherford Appleton


  1. A latchup topology to investigate novel particle detectors Alessandro Gabrielli a , Mauro Lolli a , Giulio Villani b , Danilo Demarchi c , Antonio Ranieri d a I.N.F.N. and Physics Department University of Bologna b STFC Rutherford Appleton Laboratory (RAL), UK c Laboratorio ChiLab, Engineering Department, Politecnico di Torino d I.N.F.N. and Physics Department University of Bari Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 1

  2. Outline • Introduction to the Latchup Effect • First tests via commercial BJTs • Collaboration: Bologna, RAL (STFC) , Poli_Turin – Use of MOS transistors • The CREE 24010 SiC MESFET Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 2

  3. What the “Latchup Effect” is Basically, it is an ingnition af a parasitic thyristor-like structure within a CMOS device and is ignited by induced charges inside the silicon whatever their origin. Traditional CMOS technologies into radiation environments may be susceptible and damaged by latchup Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 3

  4. First study since 2005 If (Vwell is VDD) and (Vbulk is GND) then …. It is not a reverse-biased diode plus the transistor has an internal current gain Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 4

  5. A Prototype Commercial components Q1: PNP BC858C Q2: NPN 2N3055 “ MJ21194 “ BFY52 “ 2N2222A R N : multiturn variable resistors Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 5

  6. Spice simulation (Q2=BFY52) Temperature from 30 to 40 o C 700ns 5µA × 2ns = 10fC Out Voltage Bulk Current Well Current Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 6

  7. Commercial bipolars used Q2 = 2N2222A BFY52 2N3055 TO-39 metal can TO-18 metal can TO-3 metal can Estimated B-E Estimated B-E Estimated B-E charge collection charge collection charge collection area area area 100 ÷ 10000 µm 2 10 ÷ 100 µm 2 1 mm 2 Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 7

  8. Prototype Construction (Q2=MJ21194) Metal box with upper sensor MJ21194 opening The latchup circuit inside the box Transistor Base-Emitter bondings of the power bjt MJ21194 Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 8

  9. Laboratory test Estimated sensitivity: ≈ 1pC Out signal Transistor B-E 1pC-estimated injected charge Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 9

  10. BJT to MOS transistors All that has been investigated via bipolar transistors (BJT) can be obtained using Metal-Oxide Semiconductor (MOS) transistors Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 10

  11. Here is how to use individual commercial MOS transistors (74HC04) NO VDD NO GND ..with some difficulties, honestly Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 11

  12. The schematic for many configuration and tuning capabilities 74HC04 Jumpers Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 12

  13. The Test-Board for MOS transistors Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 13

  14. Single Latchup ignition - Blue line is the N-MOS drain (P-MOS gate) - Green line is the P-MOS drain (N-MOS gate) On this line a OverSpike is provided Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 14

  15. Cyclic Latchup ignition (T=5 µ s) RESET – IGNITION OVERSPIKE - RESET – IGNITION OVERSPIKE Reset Output Ignition OverSpike - Blue plot is the N-MOS drain (P-MOS gate), “ Output ” (1V/div) - Green plot is the P-MOS drain (N-MOS gate) with the “ Ignition OverSpike” (20mV/div) - Violet plot is a cyclic “ Reset ” with a 5 µ s period (1 µ s/div) No sooner the ignition OverSpike arrives than the circuit latches Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 15

  16. Cyclic Latchup ignition (T=5 µ s) LEFT PICTURE RIGHT PICTURE - The ignition OverSpike is too weak - The ignition OverSpike is high enough - Only a few % of the times the circuit - Most of the times the circuit latches latches Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 16

  17. Noise Figure for MOS- Summarized S-curve 640 µ V Falling S-curve 1 Baseline + OverSpike Rising S-curve 0 11.44 9.68 10.80 9.84 OverSpike Input Voltage (mV) - A biasing gate baseline of about 950mV was used - Raising curve has an noise figure estimated in ≈ 640 µ V, SAY LOWER THAN 1 mV - The S-curve has an hysteresis - The estimated sensitivity, by measuring the input impedence, was confirmed to be ≈ 1pC Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 17

  18. The CREE 24010 SiC MESFET via latchup topology Spice-simulated via JFET model Actual circuit via MESFET CREE 24010 Mounted on test-board Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 18

  19. The CREE 24010 SiC MESFET via latchup topology Spice Simulations Oscilloscope plots Output on MESFET’s drain MESFET’s gate Input Spike Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 19

  20. The CREE 24010 SiC MESFET via latchup topology OUT RESET IN GATE Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 20

  21. CONCLUSION Using commercial state-of-the-art MOS transistors we have obtained: - an Error Figure of about 640µV, - a sensitivity of the order of 1pC, confirmed like for BJTs, - a readout speed of the order of 1µs. Using commercial SiC MESFET transistors we have confirmed the topology and the latchup ignition obtained with BJTs and MOSs Latchup Mechanism can be exploited in future applications for : - particle detection in high-energy physics, - radiation monitoring, - high-temperature, rad-hard applications for SiC Advantages: SIMPLE and LOW POWER An integrated version is required since 2005 ……to go ahead Alessandro Gabrielli TWEPP -2009 21-25 Sept. 2009 21

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