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NINO RO chip qualification with the laser test system Sakari and Fadmar.
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Transcript of NINO RO chip qualification with the laser test system Sakari and Fadmar.
NINO RO chip qualification with the laser test system
Sakari and Fadmar
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -2-
Diode specifications - reminder
• Pixelized diode from the IRST wafer– 200 um thickness– 300 um x 300 um pixel dimension (nominal)– 3 x 20 pixel matrix– 1 pixel under study neighboring pixels grounded– An opening in the Al-layer covering the p+-pad etched to
allow laser illumination
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -3-
Opening in the Al-layer
• From the previous measurements it was seen that there’s a big uncertainty on focusing the laser beam into the diode
A better mechanical stability was achieved An opening in the Al-layer of the diode to provide better
photon injection was etched• The opening was made by Serge Ferry (chemical lab)
– The hole was done with chemical etching. A photo-resist was placed to protect the rest of the Al-layer. The diameter of the opening is ~100 um
• With the opening the laser may be manually scanned to the center providing a maximum photon injection
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -4-
Opening in the Al-layer
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -5-
IRST diode pixelized and wire-bonded
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -6-
Connection to the NINO chip
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -7-
Laser position scan
The higher the pulse width, the more photons enter the diode, meaning thelaser is better focused to the hole
The dark red color shows the ‘hot spot’, meaning the center of the hole. The redcircle shows the assumed ~100um diameter hole.
To make sure all the photons are injected in to the diode, the laser beam is manually focused by measuring the output pulse width at different positions.
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -8-
Height scan
Laser fibre heigt scan
7
7.5
8
8.5
9
9.5
18.4 18.6 18.8 19 19.2 19.4 19.6 19.8
height of the laser fibre [100 um]
pu
lse
wid
th [
ns
] SATURATION
Complete illumination with the laser light
calibration possible using an ALICE SPD assembly (same sensor specifications)
Measurements
Laser Calibration
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -10-
Calibration of the laser light
• Reminder: W/O calibration between the laser and input charge the measurements with a calibration capacitance and the diode are incomparable
• BUT!!! Cross calibration possible with an Alice SPD assembly
• Assumptions: – The complete laser beam illuminates the detector demonstrated
(plateau reached in the fiber height scan)– Sensors of the ALICE SPD assemblies have the same specifications
as the detector under study they come from Si-wafers with same specifications
• Response of the ALICE SPD assembly to two different radioactive sources (109Cd and 55Fe) calibrates the laser beam at different settings
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -11-
Pulse Area vs Laser Bias
Laser Calibration Optical head
0
500
1000
1500
2000
2500
3000
3500
4000
4500
1.45 1.50 1.55 1.60 1.65 1.70 1.75 1.80 1.85 1.90 1.95 2.00 2.05
Laser Bias [V]
Pu
lse
area
[p
Vs]
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -12-
Laser Calibration
Laser Calibration
0.00
10000.00
20000.00
30000.00
40000.00
50000.00
60000.00
70000.00
80000.00
1.45 1.50 1.55 1.60 1.65 1.70 1.75 1.80 1.85 1.90 1.95 2.00 2.05
Laser Bias [V]
ge
ne
rate
d e
-h-p
air
s [
mV
]
extrapolation 1.48 - 1.50 V
Scaling via pulse area to 1.48 V
Scaling via pulse area to 1.50 V
Measurements
Laser Bias Scan
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -14-
Jitter
Jitter vs. input charge(w/ opened detector,no time-walk correction)
Jitter vs. laser bias(w/ detector,no time-walk correction)
Laser bias (V)
300ps300ps
Laser bias (V)
2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -15-
Jitter
Jitter vs. input charge(w/ opened detector,no time-walk correction)
Jitter vs. laser bias(w/ 100fF calibration capacitanceno time-walk correction)
Laser bias (V)
50ps300ps
2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -16-
Pulse Width
Pulse width vs. laser bias(w/ opened detector)
Pulse width vs. laser bias(w/ detector)
Laser bias (V) Laser bias (V)1.5 2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
1.5 2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -17-
Pulse Width
Pulse width vs. laser bias(w/ opened detector)
Pulse width vs. laser bias(w/ 100fF calibration capacitance)
Laser bias (V)1.5 2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -18-
Time-walk vs. Pulse width
Time-walk vs. Pulse width(w/ opened detector)
Time-walk vs. Pulse width (w/ detector)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -19-
Time-walk vs. Pulse width
Time-walk vs. Pulse width(w/ opened detector)
Time-walk vs. Pulse width (w/ 100fF calibration capacitance)
Measurements
Detector Bias Scan
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -21-
Pulse width and Jitter
Pulse width vs. detector bias(w/ opened detector)
Jitter vs. detector bias(w/ opened detector)
=~3 MIPs =~3 MIPs
Measurements
NINO Threshold Scan
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -23-
Jitter as function of the NINO threshold for 3 different laser bias settings
jitter
0.00
50.00
100.00
150.00
200.00
250.00
300.00
350.00
400.00
450.00
45 65 85 105 125 145 165 185 205 225
NINO threshold [mV]
jitte
r [p
s]
Laser Bias 1.8 V
Laser Bias 1.7 V
Laser Bias 2 V
1
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -24-
Conclusions
• Mechanical stability achieved– New precision mechanics installed– NINO board fixed to a reference plane – repeatability tested and improved system mechanically stable
• Opening in the Al-layer allows the complete illumination with the laser light– Procedure established with TS/DEM group – Verified on 5 samples openings range from 100 um – 3 mm– laser calibration finally! possible
• Measurements on the NINO chip show improved results: jitter <200 ps for high det-bias and >1.8 V laser bias (~3 MIPs)– With the current RO-setup (detector wire-bonded to the NINO chip,
no pre-amp) NO further improvement possible!– Next step: demonstrator
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -25-
SPARE SLIDES
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -26-
Jitter Comparison 1pF
Jitter vs. input charge(w/ opened detector,no time-walk correction)
Jitter vs. laser bias(w/ 1pF calibration capacitanceno time-walk correction)
Laser bias (V)
300ps300ps
2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -27-
Pulse Width Comparison 1pF
Pulse width vs. laser bias(w/ opened detector)
Pulse width vs. laser bias(w/ 1pF calibration capacitance)
Laser bias (V)1.5 2.6 3.6 4.7 6.3 7.3 8.3 9.2 10 10.7
Generated charge (fC)
Fadmar Osmić – P326 GTK Meeting, December 11, 2007 -28-
Time-walk vs. Pulse widthComparison 1pF
Time-walk vs. Pulse width(w/ opened detector)
Time-walk vs. Pulse width (w/ 1pF calibration capacitance)