The Sensor Test for CMS pixel upgrade
Introduction
The Compact Muon Solenoid, CMS, is a general purpose detector for the Large Hadron Collider,
LHC, accelerator at CERN. The CMS tracker, the innermost part of the CMS detector,
is composed of a pixel detector with three barrel layers at radii
between 4.4cm and 10.2cm and a silicon strip tracker with 10 barrel detection layers extending
outwards to a radius of 1.1m. Each system is completed by endcaps which consist of 2 disks in
the pixel detector and 3 plus 9 disks in the strip tracker on each side of the barrel, extending the
acceptance of the tracker up to a pseudorapidity of |eta|< 2.5.
After 2-3 years of operating at LHC the performances of the innermost barrel layer sensors
will degradate significantly due to radiation damage. For this reason a replacement of the whole
pixel detector is scheduled for 2013 in conjunction with the shutdown for Phase I upgrade.
The sensors for the CMS-pixel detector adopt the so called n-on-n concept. The pixels consist
of high dose n-implants introduced into a high resistance n-substrate. The rectifying pn-junction
is placed on the back side of the sensor surrounded by a multi guard ring structure. Despite the
higher costs due to the double sided processing this concept was chosen as the collection of electrons
ensures a high signal charge at moderate bias voltages (< 600V) after high hadron fluences.
Furthermore the double sided processing allows a guard ring scheme keeping all sensor edges at
ground potential.
The sensor quality is tested through the leakage current vs. bias voltage measurement.
The current-to-voltage curve has an obvious charactersistic. For the voltages below full depletion the
current increases proportional to the square root of the bias. When the space charge reaches a structured
backside, an additional surface contribution arises. After full depletion the IV-curve displays a plateau region in which
the current increase is very small before electrical breakdown occurs at very high voltages. Almost all possible problems
in the sensor production process lead to a deviation of the curve from the expected shape.
the Instruments Setup
- a PC, communicate with the Keithley source meter and the prober station
- a Keithley 2410 source meter, supply the voltage
- a prober station SUSS PA200, has a 3-groove chuck fixing the sensors and two needles touching the sensors
the Labview VI
The move_meas.vi is designed to integrate the chuck movement and IV measurement.
Its front panel looks like,
The values of x, y, z and sensor No. should be set before mesurement.
The (x,y,z) means chuck's position, which should be precisely pre-tested to make sure the two needles touch the small square pads on the sensor.
If the groove has sensor, choose "on"; otherwise choose "off".
The data is saved in the given "path".
On the bottom the error-outs show the error information for initialization, load back, movements and I-V measurements.
The default voltage setup is from 0~-600v with each step -5v and waiting time 1s. The alarm current limit is 100uA.
These values can be changed in the subVI sensor_IV_measurement.vi .
Tips
The first chuck point's z value is better to be larger than 1500um before fix the needles.
The z relative values can be obtained by adjusting the chuck to microscope's focus distance while fixing scope height.
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XiaWan - 04-May-2011