Construction and first beam-tests of silicon-tungsten prototype modules for the CMS High Granularity Calorimeter for HL-LHC
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1 TIPP May 2017, Beijing Construction and first beam-tests of silicon-tungsten prototype modules for the CMS High Granularity Calorimeter for HL-LHC Francesco Romeo On behalf of the CMS collaboration
2 Introduction Motivation for the High Granularity Calorimeter (HGCal) in HL-LHC In the High-Lumi (HL) LHC era, we need to maintain: smoothly running detector high quality object reconstruction/identification Extreme conditions in endcap region High radiation (up to n/cm 2 at η 3) High pileup ( ) Use silicon-based HGCal detector Radiation tolerant High granularity and fast timing For more motivations, please refer to talk by Florian Michael Pitters francesco.romeo@cern.ch (IHEP Beijing) Pag 1 / 17
3 HGCal overview Introduction More on HGCal in the talk by Florian Michael Pitters (IHEP Beijing) Pag 2 / 17
4 Introduction 2016 beam-tests at FNAL and CERN Primary goals: Proof of concept of the baseline HGCal design with a closely spaced stack-up of modules Validation of the overall design concept of a hexagonal silicon sensor mounted on a baseplate with a PCB with holes for the wire-bonding Performance of silicon-tungsten prototype modules: Studies: Pedestal and noise Single particle calibration Measurements: Longitudinal and transverse shower shapes Energy, position, time resolution Compare results with simulation francesco.romeo@cern.ch (IHEP Beijing) Pag 3 / 17
5 Setup Hexagonal Si-Sensor (128 channels) (IHEP Beijing) Pag 4 / 17
6 Module assembly Setup (IHEP Beijing) Pag 5 / 17
7 Setup Data Acquisition System Use commercial components mounted on custom PCBs (IHEP Beijing) Pag 6 / 17
8 Setup Data taking setup & conditions FNAL CERN 16 modules, 15 X0 8 modules, 5-27 (6-15) X0 e beam (4-32) GeV e beam (20-250) GeV p beam 120 GeV π(µ from π) beam 125 (120) GeV francesco.romeo@cern.ch (IHEP Beijing) Pag 7 / 17
9 Pedestal and noise stability Studies From CERN test with 8 layers (16 Skiroc2 ASICs) Pedestal and noise stable within 2 ADC count (1 ADC 1/17 MIP) francesco.romeo@cern.ch (IHEP Beijing) Pag 8 / 17
10 Electron beams: event display Studies (IHEP Beijing) Pag 9 / 17
11 MIP calibration Studies FNAL: p beam 120 GeV CERN: π(µ from π) beam 125 (120) GeV Calibrate only central cells of sensor within trigger area Variations due to the electronic and cell size francesco.romeo@cern.ch (IHEP Beijing) Pag 10 / 17
12 Measurements Transverse and longitudinal shower shapes Excellent agreement between measurements and simulation one of the main goals achieved (IHEP Beijing) Pag 11 / 17
13 Energy resolution Measurements Energy measured in the silicon layers plus sampling factors for the absorbers Wide range of energies covered FNAL, CERN trends VS energy reflect different sampling regimes Limited longitudinal samplings limit the achievable electron energy resolution Good agreement between data and simulation (IHEP Beijing) Pag 12 / 17
14 Position resolution Measurements Measure the difference between a track extrapolated from two wire chambers (upstream of first HGCal module) and the shower position (logarithmic weight E 19 cell) Precision of a few mm can be achieved It increases with energy and decreases with depth in calorimeter Good agreement with simulation francesco.romeo@cern.ch (IHEP Beijing) Pag 13 / 17
15 Time resolution Measurements (IHEP Beijing) Pag 14 / 17
16 Outlook & Summary HGCal beam test in 2017 (Goal 1) Updated front-end chip, Skiroc2-CMS, featuring HGCal ASIC: 25 ns peaking time ( 200 ns in SKIROC2) Time Over Threshold (ToT) for large signals Time of Arrival information ( 50 ps timing) to explore timing performance Single layer PCB to achieve the desired compactness For more details, see talk by Johan Borg New DAQ required First beam-test on a single module successfully completed in May francesco.romeo@cern.ch (IHEP Beijing) Pag 15 / 17
17 Outlook & Summary HGCal beam test in 2017 (Goal 2) (IHEP Beijing) Pag 16 / 17
18 Summary Outlook & Summary HGCal is the CMS decision for replacing its current endcap in HL-Lumi era: Good energy resolution for electromagnetic and hadronic particles in an extremely high-radiation environment High granularity and fast timing to deal with high pileup Proof of concept through construction and first beam-tests of silicon-tungsten prototype modules Measured resolution for: Energy: below 7%, for e energy > 50 GeV Position: below 2mm, for e energy > 50 GeV Time: 20 ps Basic validation of the simulation In 2017 campaign, we aim to study full system performance (EE+FH+BH) francesco.romeo@cern.ch (IHEP Beijing) Pag 17 / 17
19 Fullly assembled module Backup (IHEP Beijing) Pag 18 / 17
20 Data taking setup Backup (IHEP Beijing) Pag 19 / 17
21 High gain - Low gain correlation Backup High gain saturation around [1800;200] ADC in [HG;LG] plane HG/LG ratio 10 francesco.romeo@cern.ch (IHEP Beijing) Pag 20 / 17
22 Backup (IHEP Beijing) Pag 21 / 17
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