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Matteo VIGNETTI *a (WP2 ESR PhD Student)

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Presentation on theme: "Matteo VIGNETTI *a (WP2 ESR PhD Student)"— Presentation transcript:

1 Matteo VIGNETTI *a (WP2 ESR PhD Student)
*Supported by the European Union’s Seventh Framework Programme for research, technological development and demonstration under grant agreement n° 317446 (INFIERI) Update on the development of Novel Pixel Sensors based on 3D CMOS technology Matteo VIGNETTI *a (WP2 ESR PhD Student) F. Calmon a(Supervisor), R. Cellier b, P. Pittet b, L. Quiquerez b, A. Savoy-Navarro c a Electronic Devices Department, INL, Lyon (France) b Conception de Systèmes Hétérogènes, INL, Lyon (France) c Laboratoire d’AstroParticule et Cosmologie, Université Paris-Diderot, Paris (France)

2 A novel 3D pixelated detector for vertex tracking
A 3D pixel: the core of the detector p p Two coincident avalanche pulses are produced when a charged particle hits the pixel Two vertically aligned avalanche diodes operated in Geiger-mode The coincidence is verified thanks to dedicated electronics e h p p TOP = 1 OUT = 1 BOTTOM = 1 e h p p p

3 Coincidence-based Avalanche Detector concept
In particles tracking systems, the ideal detector should provide a large signal while featuring a thin sensitive volume Geiger-mode avalanche diodes: A very thin sensitive region (~𝜇𝑚) is enough to produce a strong electrical signal thanks to a self-sustained multiplication process by impact ionization suffer of false counts (dark count rate), due to dark thermal and field-assisted e/h pair generation and background photons Coincidence detection: Dramatically reduces the amount of false counts as the DCR of the two diodes are uncorrelated false counts might occur during the time-window where the coincidence is checked (Typical CMOS tech) X 𝟏𝟎 𝟒 improvement 𝐹𝐶𝑅=2𝐷𝐶 𝑅′ 2 𝐴 2 ∆𝑡 FCR:Fake coincidence rate 𝐷𝐶𝑅′: dark count rate of the diode per unit surface A: diode active area

4 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

5 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

6 Design of the avalanche diode
Premature edge breakdown (PEB) prevention Sensitive surface Cathode Anode PEB! OK! Dark Count Rate (DCR) minimization DCR depends on the e – h pair generation rate in the diode space charge region (in the dark) Carrier generation rate depends on: CMOS technology (i.e. defects density) avalanche diode architecture (e.g. junction enhancing tunneling-based carrier generation)

7 Design of the avalanche diode
TCAD simulations of several avalanche diode architectures found in literature: AMS HV-CMOS 0,35µm technology “low doped p-well guard-ring” Substrate Choice of the architecture based on: Affordable CMOS technology in terms of tape-out costs Best performing architecture among those compatible with the chosen CMOS technology 𝟓𝟎𝝁𝒎 Anode Cathode

8 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

9 Design of the pixel electronics – 2D level
Geiger-mode operation: - - // - - 𝑽 𝑫 𝑰 𝑫 l 𝑽 𝒃𝒅 𝑽 𝒃𝒊𝒂𝒔 = 𝑽 𝒃𝒅 + 𝑽 𝒆𝒙 𝑰 𝑫 𝐢𝐬 𝐧𝐨𝐰 ~ 𝟎 𝑨, hence working point moves back to 𝑽 𝑫 = 𝑽 𝒃𝒅 + 𝑽 𝒆𝒙 Impinging photon at 𝑡= 𝑡 0 𝑽 𝑫 𝑰 𝑫 𝑽 𝒃𝒅 + 𝑽 𝒆𝒙 𝑹 𝑳 Working point at or below 𝑽 𝒃𝒅 Quenching Avalanche Initial bias 𝑽 𝒃𝒅 + 𝑽 𝒆𝒙 l Recharge to the initial bias 𝒕 𝑽 𝒐 𝑽 𝒐 =𝟎𝑽 𝒕 𝒊 l 𝒕 𝟎 𝑽 𝒐 = 𝑽 𝒆𝒙

10 Design of the pixel electronics – 2D level
A time integration-base passive quench - active recharge circuit Vignetti M. et al “A time-integration based quenching circuit for Geiger-mode avalanche diodes” 13th IEEE International New Circuits and Systems Conference (NEWCAS 2015) June 7-10, 2015 Grenoble, France (2015)

11 Design of the pixel electronics – 3D level
The 3D pixel electronics has to be conceived in order to account for the possible parasitics introduced by the vertical interconnections. SET_CoincidenceWindow Coincidence_OUT Coincidence circuit Pulse shaping circuit Bottom TIER 3D interconnection Top TIER Coincidence circuit 3D Pixel SET_CoincidenceWindow

12 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

13 3D integration Dedicated 3D technologies Flip-chip assembly VS Source: Tezzaron Parasitics Bump-bond based assembly Large bump diameter Chip-level assembly: Affordable! negligible parasitics very large scale integration compatible (𝑑~1𝜇𝑚) Wafer level  very expensive! 3D integration strategy: TOP tier and BOTTOM tier on the same chip! Only external PADs on BOTTOM die will be wire-bonded

14 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

15 Tape-out A test-chip submitted for TAPE-OUT on April 23rd in a MPW run. Chips received on mid-September 2015 3D pixels cells 2x2 hybrid matrix cells Test structures

16 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

17 Preliminary tests Signal analysis Test setup Setup is good for
Daughter board Setup is good for Simple preliminary tests to check the different circuits and test structures Some nice measurements can be obtained with a good oscilloscope But It is not practical for a full characterization Parasitics Dedicated testing board is required!

18 Preliminary tests Tunable hold-off time
154ns 44ns Potentially short hold-off time A dark count followed by an after-pulse 29ns

19 Preliminary tests Coincidence between two on-plane diodes
𝑉 𝑒𝑥 =1 𝑉 and 𝑡 ℎ = 75 𝑛𝑠 : diode “bottom” (left)  38 kHz (15,2 𝐻𝑧/𝜇 𝑚 2 ) diode “top” (right)  16,8 kHz (6,7 𝐻𝑧/𝜇 𝑚 2 )  Results are similar to what it is found in literature After-pulsing is negligible for 𝑡 ℎ >200𝑛𝑠 Estimated FCR = 13 Hz OBS:calculated FCR (not measured!). Measurements show a negligible amount of fake pulses in a wide acquisition window in the oscilloscope. Accurate measurements not yet available due to oscilloscope and test-bench limitations

20 Outline Design of the avalanche diode Design of the pixel electronics 3D integration Tape-out Preliminary tests Design of a testing board

21 Design of a testing board
Signal analysis Custom PCB board FTDI (FPGA) USB Daughter board

22 Conclusions A PEB safe avalanche diode has been designed accounting for the technological limitation imposed by the adopted CMOS process Dedicated electronics for both Geiger-mode operation as well as coincidence detection have been devised A 3D coincidence-based pixel as well as a small hybrid matrix has been successfully designed. Test-chip submission for tape-out has been successfully accomplished Preliminary results on functionality check are goods. A dedicated test board design for an optimal characterization is in progress

23 Thanks!


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