Setup for measurements with SCT128 in Ljubljana: SCTA128VG chip

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Presentation transcript:

Setup for measurements with SCT128 in Ljubljana: SCTA128VG chip drawings of test pcb from CERN (thanks to Jan Kaplon) VME module SEQSI (for clock, commands...) Tektronix digital scope for data acquisition Cambridge LabView software for chip control (thanks to Dave Robinson) data acquisition software (thanks to G. Kramberger ) pitch adapters from Freiburg (thanks to Uli Parzefal) coincidence circuit made by Erik Margan 90Sr source, photomultiplier, scintillator, power supplies.... I. Mandić, SCT128 mesurement setup

Test PCB Detector (1.2x1.2 cm2) SCTA128VG Fanin Al detector support and heat spreader PT100 I. Mandić, SCT128 mesurement setup

Scintillator is under the Aluminium support structure dimensions: ~ 25 cm x 20 cm x 6 cm 90Sr source is inserted into the upper collimator Test board holder Scintillator is under the lower collimator Photo Multiplier Light guide I. Mandić, SCT128 mesurement setup

Setup in the freezewr, temperature about - 20° C 90Sr source holder I. Mandić, SCT128 mesurement setup

charge sensitive front-end amplifier with about 20 ns peaking time SCTA128VG chip 128 channels charge sensitive front-end amplifier with about 20 ns peaking time sampled every 25 ns (40 MHz sampling clock) Gain = 26.5 mV/fC = 4.2 µV/el measured with calibration signals from on-chip capacitors (~10 % accuracy) noise with detector connected ~ 800 el Strips bonded I. Mandić, SCT128 mesurement setup

p-type, FZ material, 300 µm thick miniature (~ 1 cm2) strip detectors strip pitch 80 µm n-in-p capacitively coupled polysilicon biased, p-sprayed designed by Liverpool produced by Micron CV measurement, contact through bias ring I. Mandić, SCT128 mesurement setup

fitted with convolution of Landau and Gauss functions Measurements trigger: signals caused by electrons from 90Sr source in scintillator in coincidence with 40 MHz clock edge spectrum of signals from strips (pedestals and common mode variations subtracted) fitted with convolution of Landau and Gauss functions  “Most Probable Value” of the Landau function (parameter p1 in the plot below) returned by the fit is the measure of collected charge Bias = 350 V I. Mandić, SCT128 mesurement setup

signal mean vs. trigger delay, before irradiation Bias = 200 V Pulse shape signal mean vs. trigger delay, before irradiation Bias = 200 V I. Mandić, SCT128 mesurement setup