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Silicon pad detector for an electromagnetic calorimeter at future linear collider experiments: characterisation and test beam results Antonio Bulgheroni University of Milan – Italy on behalf of LCCAL: Official INFN R&D project, official DESY R&D project PRC R&D 00/02 Contributors (Como, LNF, Padova, Trieste): M. Alemi, M.Bettini, S. Bertolucci, E. Borsato, M. Caccia, P.Checchia, C. Fanin, G. Fedel, J. Marczewski, S. Miscetti , M. Nicoletto, M. Prest, R. Peghin, L. Ramina, E. Vallazza. 8th ICATPP – Villa Erba (Como), 6th October ‘03 Calorimeter Layout Absorber 25 x 25 x 0.3 cm3 Scintillator 25 Cells 5 x 5 cm2 Silicon pad detectors Total of 50 layers 27 X0 3 layers 725 Pads ~ 1 x 1 cm2 2, 6 and 12 X0 Main characteristics: Sensor thickness: 300mm Resistivity: 4-6k AC coupling (2 ways) Silicon dioxide thickness: 265 nm SMD capacitors Bias grid and guard ring 3M poly-Si bias resistors Symmetric structure ~0.9 cm 6 cm 7 cm 8th ICATPP – Villa Erba (Como), 6th October ‘03 Sensor details ~0.9 cm Bias pad Guard ring pad 8th ICATPP – Villa Erba (Como), 6th October ‘03 Hybridisation details Hybridisation through conductive glue Analogue Readout Chip: VA-HDR9c (IdeAs) SMD caps VA Viking family HDR High dynamic range 9c Four selectable gains Gain* [mv/fC] DR [mip] 3.3 2.5 1.7 1.2 ± 100 ± 140 ± 200 ± 300 *Measured value 8th ICATPP – Villa Erba (Como), 6th October ‘03 Motherboard design 6 sensors per motherboard with serial readout. Status of production: 24 sensors available 3 motherboards fully and 2 partially equipped Signal routing through Erni connectors 8th ICATPP – Villa Erba (Como), 6th October ‘03 How we get there… step by step 3 technological runs First batch of 11 sensors (spring ’02) Next batch will be ready next months GOOD! Third batch of 9 sensors (summer ’03) Soft Breakdown Second batch of 9 sensors (summer ’02) “Leaky” pads 8th ICATPP – Villa Erba (Como), 6th October ‘03 Soft breakdown Bias current reasonable (few mA) Strange shape with a “soft” breakdown n+ or metal shallow impurities on the backplane Depletion region n Solution 1: replace the implanted backside contact with a diffused one, but it does not work! n+ Solution 2: replace the mash backplane contact with a uniform one, it works! Metal Impurities No pin holes in SiO2 Surface leakage residua of polysilicon after the etching of the polysilicon layer Equivalent circuit with two opposite diodes. C D1 Al bridge Readout Polysilicon metal residua Resistor D2 R D 8th ICATPP – Villa Erba (Como), 6th October ‘03 “Leaky” pads: a surface effect p+ Solution: remove the integrated capacitors n Bias grid 8th ICATPP – Villa Erba (Como), 6th October ‘03 Yield Quite uniform behaviour of the depletion voltage YIELD 1st Batch 2nd Batch 3rd Batch Coupling AC AC DC Wafer Rejected 1/11 2/9 0/9 Depletion Voltage 32V 27V 28 V Current @ depletion 2.1 mA 0.8 mA 0.6 mA Not depleted pads 0/420 8/249 0/378 8th ICATPP – Villa Erba (Como), 6th October ‘03 Test beam: Signal to Noise ratio Theory: ENC A ENC e q e ENC q B pF 1000e + qI lTp 30e 4 + 2nd batch: ~ 15 T p k BT 2R 1st batch: ~ 10 230e = 1260e Theoretical* SNR ~ 20 *Value obtained for detector of the 3rd batch 3rd batch: ~ 18 8th ICATPP – Villa Erba (Como), 6th October ‘03 Test beam: shower reconstruction / 1 20 GeV e@ 2X0 Forward tracker @ 6X0 @ 12X0 8th ICATPP – Villa Erba (Como), 6th October ‘03 Test beam: shower reconstruction / 2 20 GeV e@ 2X0 Forward tracker @ 6X0 @ 12X0 8th ICATPP – Villa Erba (Como), 6th October ‘03 Test beam: energy linearity Silicon wafers rearranged in 5 planes ant tested alone Pb of 2.5 cm Electrons beam Error bars = sigma distribution 8th ICATPP – Villa Erba (Como), 6th October ‘03 Summary Some technological problems fixed with the last batch Detector performances very close to the design rules and hopefully will improve with the next and last batch Shower reconstruction capability and energy linearity are shown in the first test beam … we keep going …