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Preliminary results from 3D CMS Pixel Detectors

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Presentation on theme: "Preliminary results from 3D CMS Pixel Detectors"— Presentation transcript:

1 Preliminary results from 3D CMS Pixel Detectors
Ozhan Koybasi1, E. Alagoz1, K. Arndt1, D. Bortoletto1, I. Shipsey1, G. Bolla1, T. E. Hansen2, A. Kok2, T. A. Hansen2, N. Lietaer2, G. U. Jensen2, A.Summanwar2, R. Riviera3, M. Turqueti3, L. Uplegger3, and S. W. L. Kwan3 1Physics Department, Purdue University, West Lafayette, IN 47907‐2036 USA 2SINTEF, SINTEF MiNaLab, Blindern, 0314 Oslo, Norway 3Fermilab, Batavia, IL 60510‐5011 USA 16th RD50 Workshop ,Barcelona, June 2nd , 2010 1

2 3D Detectors - CMS Pixel Layouts
First fabricated at Stanford Nanofabrication facility in 1997 As a part of “3D Collaboration” , fabrication transferred to SINTEF for small and medium scale production Two different 3D CMS layouts: - 4 readout electrodes per pixel (4E) - 2 readout electrodes per pixel (2E) 2E Configuration 4E Configuration n+ (readout) electrodes p+ (bias) electrodes 100 µm More radiation hard: 150 µm Faster response Lower depletion voltage Less trapping Lower noise Larger active volume 2

3 Wafer Layout p-type wafers with resistivity > 10 kΩ.cm Two different wafer thicknesses: - B5 : 280μm thick - B2-16 : 200μm thick Include ATLAS, CMS, and MediPix devices MediPix chips 3

4 Wafer bonding by direct fusion bonding
Fabrication at SINTEF p-spray isolation : 6x1012cm-2, 60keV, through a 60nm oxide. Annealed at 900oC for 30 minutes Wafer bonding by direct fusion bonding Deep Reactive ion etching (DRIE) & polysilicon filling and doping of electrodes - n-type electrode etching & filling (diameter of 14 µm) - 300nm thermal oxide barrier protection - p-type electrode and active edge etching & filling (5 µm active edge) Metal layer deposition & patterning Passivation layer of 0.5µm oxide and 0.25µm nitride deposition by PECVD & patterning 4

5 Assembly & Wire-bonding
bias wire Support wafer made wire-bonding challenging ( especially high voltage wiring) Carbon fiber Cooling done by a chiller Sensor temperature measurement: an RTD placed on the carbon fiber (cooling tubes side): ΔΤ = 6 °C sensor Cooling tubes Base plate VHDI Adhesive ROC Sensor Bump bonds Support wafer Bias wire Wire bond Au plate Ceramic plate Bias pad 5

6 T = 21°C I-V Characteristics 6 Detector I (@40V) [μA] / Chip
[nA] / Pixel Breakdown Voltage [V] 2E-WB5-2 0.7 0.35 120 2E-WB2-16-6 5 2.5 4E-WB5-8 2 1 100 4E-WB2-16-5 10 6

7 Noise Tests Noisy edges Measured at room temperature Unable to measure noise at Vbias < 40V for 4E sensors 2E Wafer B5 #2 Vbias = ‐40 V 7

8 Bump bond tests @ Vbias=40V
2E Wafer B5 #2 2E Wafer B2‐16 #6 4E Wafer B2‐16 #5 4E Wafer B5 #8 8

9 CLOCK AND TRIGGER DISTRIBUTION
Test Beam Set Up at FNAL TELESCOPE ENCLOSURE BEAM FERMILAB NETWORK CONTROL ROOM DUT PIXEL DETECTORS SCINTILLATORS 3.7V POWER SUPPLY ACELLERATOR CLOCK CLOCK AND TRIGGER DISTRIBUTION 2x3 plaquettes 120 GeV protons No B field 2x4 plaquettes CAPTAN SYSTEM 9

10 Beam Test Results: 2E_WB5_2
Beam spot on 3D ADC to electron conversion: Vcal* [DAC] = ADC x gain - offset Charge (e-) = Vcal x 65.5 – 410 * 1 Vcal [DAC] = 65.5 electrons T ≈ 11 oC on carbon fiber (estimated to be 6 oC higher on the sensor) Threshold [DAC]= 50 Vbias = 40V 10

11 Beam Test Results: 2E_WB5_2
Threshold [DAC] = 50 Vbias=40V Each point is charge distribution mean Most probable value to be determined after re-doing gain calibration Electron equivalence of threshold to be determined with CAPTAN system 11

12 Beam Test Results: 2E_WB2-16_6
Gain calibration needed ADC distribution Beam spot on 3D Vbias=40V 12

13 - Good I-V behavior except one 2E sensor
Summary and Future plans Bump-bonded 3D CMS pixel sensors with 2E and 4E configurations assembled into plaquettes and characterized. - Good I-V behavior except one 2E sensor - High noise : ~ 450 electrons for 4E sensors and electrons for 2E sensors -Good bump-bond quality Some sensors tested at FNAL with 120 GeV protons - Bias and threshold scans of charge performed. Gain calibration to be re-done and equivalence of threshold to be determined with CAPTAN system at Purdue - Results for 2E sensors are promising while 4E sensors failed. More sensors to be studied more thoroughly with test beam at FNAL and radioactive source at Purdue before and after irradiation 13

14 BACKUP SLIDES

15 Correlation between planes

16 Threshold [DAC]= 50, Vbias = 60V
Sensor : 2E_WB5_2 DUT

17 Threshold [DAC]= 50, Vbias = 60V
DUT

18 Threshold [DAC]= 50, Vbias = 60V
DUT

19 Threshold [DAC]= 50, Vbias = 60V
DUT

20 Threshold [DAC]= 50, Vbias = 60V
Sensor : 2E_WB2-16_6 DUT

21 Threshold [DAC]= 50, Vbias = 60V
DUT

22 Threshold [DAC]= 50, Vbias = 60V
DUT

23 Threshold [DAC]= 50, Vbias = 60V
DUT


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