4.3 Article

Beam test measurements of Low Gain Avalanche Detector single pads and arrays for the ATLAS High Granularity Timing Detector

Journal

JOURNAL OF INSTRUMENTATION
Volume 13, Issue -, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/1748-0221/13/06/P06017

Keywords

Si microstrip and pad detectors; Solid state detectors; Timing detectors

Funding

  1. United States Department of Energy [DE-FG02-04ER41286]
  2. MINECO, Spanish Government (European Union's FEDER funds) [FPA2013-48308-C2-1-P, FPA2014-55295-C3-2-R, FPA2015-69260-C3-2-R, FPA2015-69260-C3-3-R]
  3. MINECO, Spanish Government (Severo Ochoa excellence programme) [SEV-2012-0234]
  4. Juan de la Cierva programme
  5. MINECO
  6. Catalan Government (AGAUR): Grups de Recerca Consolidats [SGR 2014 1177]
  7. European Union's Horizon 2020 Research and Innovation programme [654168]
  8. Cluster of Excellence Precision Physics, Fundamental Interactions and Structure of Matter of the German Research Foundation [PRISMA - EXC 1098]

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For the high luminosity upgrade of the LHC at CERN, ATLAS is considering the addition of a High Granularity Timing Detector (HGTD) in front of the end cap and forward calorimeters at vertical bar z vertical bar = 3:5 m and covering the region 2:4 < vertical bar eta vertical bar < 4 to help reducing the effect of pile-up. The chosen sensors are arrays of 50 mu m thin Low Gain Avalanche Detectors (LGAD). This paper presents results on single LGAD sensors with a surface area of 1.3 x 1.3 mm(2) and arrays with 2 x 2 pads with a surface area of 2 x 2 mm(2) or 3 x 3 mm(2) each and different implant doses of the p(+) multiplication layer. They are obtained from data collected during a beam test campaign in autumn 2016 with a pion beam of 120 GeV energy at the CERN SPS. In addition to several quantities measured inclusively for each pad, the gain, efficiency and time resolution have been estimated as a function of the position of the incident particle inside the pad by using a beam telescope with a position resolution of few mu m. Different methods to measure the time resolution are compared, yielding consistent results. The sensors with a surface area of 1.3 x 1.3 mm(2) have a time resolution of about 40 ps for a gain of 20 and of about 27 ps for a gain of 50 and fulfil the HGTD requirements. Larger sensors have, as expected, a degraded time resolution. All sensors show very good efficiency and time resolution uniformity.

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