Test beam characterization of sensor prototypes for the CMS Barrel MIP Timing Detector
Test beam characterization of sensor prototypes for the CMS Barrel MIP Timing Detector
复制标题
CMS Barrel MIP 定时探测器的传感器原型的测试光束表征
DOI:
10.1088/1748-0221/16/07/p07023
复制
发表时间:
2021
影响因子:
1.3
通讯作者:
Auffray, E.
中科院分区:
文献类型:
--
作者:
Abbott, R.;Abreu, A.;Addesa, F.;Alhusseini, M.;Anderson, T.;Andreev, Y.;Apresyan, A.;Arcidiacono, R.;Arenton, M.;Auffray, E.
The MIP Timing Detector will provide additional timing capabilities for detection of minimum ionizing particles (MIPs) at CMS during the High Luminosity LHC era, improving event reconstruction and pileup rejection. The central portion of the detector, the Barrel Timing Layer (BTL), will be instrumented with LYSO: Ce crystals and Silicon Photomultipliers (SiPMs) providing a time resolution of about 30 ps at the beginning of operation, and degrading to 50-60 ps at the end of the detector lifetime as a result of radiation damage. In this work, we present the results obtained using a 120 GeV proton beam at the Fermilab Test Beam Facility to measure the time resolution of unirradiated sensors. A proof-of-concept of the sensor layout proposed for the barrel region of the MTD, consisting of elongated crystal bars with dimensions of about 3× 3× 57 mm 3 and with double-ended SiPM readout, is demonstrated. This design provides a robust time measurement independent of the impact point of the MIP along the crystal bar. We tested LYSO: Ce bars of different thickness (2, 3, 4 mm) with a geometry close to the reference design and coupled to SiPMs manufactured by Hamamatsu and Fondazione Bruno Kessler. The various aspects influencing the timing performance such as the crystal thickness, properties of the SiPMs (eg photon detection efficiency), and impact angle of the MIP are studied. A time resolution of about 28 ps is measured for MIPs crossing a 3 mm thick crystal bar, corresponding to a most probable value (MPV) of energy deposition of 2.6 MeV, and of 22 ps for the 4.2 MeV MPV energy deposition expected in the BTL, matching the detector performance target for unirradiated devices.
DOI:
--
发表时间:
2016
期刊:
影响因子:
--
作者:
S. Kwan;CM Lei;D. Menasce;L. Moroni;J. Ngadiuba;A. Prosser;R. Rivera;S. Terzo;Marcos Turqueti;Lorenzo;Uplegger;L. Vigani;M. Dinardo
通讯作者:
M. Dinardo
DOI:
--
发表时间:
2019
期刊:
Nuclear Instruments and Methods in Physics Research Section A : Accelerators, Spectrometers, Detectors and Associated Equipment
影响因子:
--
作者:
J. Bortfeldt;F. Brunbauer;C. David;D. Desforge;G. Fanourakis;M. Gallinaro;F. García;I. Giomataris;T. Gustavsson;C. Guyot;F. J. Iguaz;M. Kebbiri;K. Kordas;P. Legou;Jianbei Liu;M. Lupberger;I. Manthos;H. Muller;Vasileios Niaouris;E. Oliveri;T. Papaevangelou;K. Paraschou;M. Pomorski;F. Resnati;L. Ropelewski;D. Sampsonidis;T. Schneider;P. Schwemling;E. Scorsone;L. Sohl;M. Stenis;P. Thuiner;Y. Tsipolitis;S. Tzamarias;R. Veenhof;Xu Wang;S. White;Zhiyong Zhang;Yi Zhou
通讯作者:
Yi Zhou