Published December 21, 2013 | Version v1
Journal article

Testbeam and laboratory test results of irradiated 3D CMS pixel detectors

  • 1. Purdue University, School of Electrical and Computer Engineering, West Lafayette, IN 47907-1396 (United States)
  • 2. Purdue University, Department of Physics, West Lafayette, IN 47907-1396 (United States)
  • 3. Istituto Nazionale di Fisica Nucleare, Sezione di Torino, 10125 Torino (Italy)
  • 4. Dipartimento di Ingegneria e Scienzadella Informazione, Universitá di Trento, I-38123 Povo di Trento (Italy)
  • 5. INFN Padova (Gruppo Collegato di Trento) (Italy)
  • 6. Universitá degli Studi di Milano Bicocca, 20126 Milano (Italy)
  • 7. Istituto Nazionale di Fisica Nucleare, Sezione di Milano Bicocca (Italy)
  • 8. Fermi National Accelerator Laboratory, Batavia, IL 60510-0500 (United States)
  • 9. Texas A and M University, Department of Physics, College Station, TX 77843-4242 (United States)
  • 10. Centro per i Materiali e i Microsistemi Fondazione Bruno Kessler (FBK), Trento, I-38123 Povo di Trento (Italy)
  • 11. Strasbourg IPHC, Institut Pluriedisciplinaire Hubert Curien, F-67037 Strasbourg Cedex (France)
  • 12. State University of New York at Buffalo (SUNY), Department of Physics, Buffalo, NY 14260-1500 (United States)

Description

The CMS silicon pixel detector is the tracking device closest to the LHC p–p collisions, which precisely reconstructs the charged particle trajectories. The planar technology used in the current innermost layer of the pixel detector will reach the design limit for radiation hardness at the end of Phase I upgrade and will need to be replaced before the Phase II upgrade in 2020. Due to its unprecedented performance in harsh radiation environments, 3D silicon technology is under consideration as a possible replacement of planar technology for the High Luminosity-LHC or HL-LHC. 3D silicon detectors are fabricated by the Deep Reactive-Ion-Etching (DRIE) technique which allows p- and n-type electrodes to be processed through the silicon substrate as opposed to being implanted through the silicon surface. The 3D CMS pixel devices presented in this paper were processed at FBK. They were bump bonded to the current CMS pixel readout chip, tested in the laboratory, and testbeams carried out at FNAL with the proton beam of 120 GeV/c. In this paper we present the laboratory and beam test results for the irradiated 3D CMS pixel devices. -- Highlights: •Pre-irradiation and post-irradiation electrical properties of 3D sensors and 3D diodes from various FBK production batches were measured and analyzed. •I–T measurements of gamma irradiated diodes were analyzed to understand leakage current generation mechanism in 3D diodes. •Laboratory measurements: signal to noise ratio and charge collection efficiency of 3D sensors before and after irradiation. •Testbeam measurements: pre- and post-irradiation pixel cell efficiency and position resolution of 3D sensors

Availability note (English)

Available from http://dx.doi.org/10.1016/j.nima.2013.07.042

Additional details

Identifiers

DOI
10.1016/j.nima.2013.07.042;
PII
S0168-9002(13)01051-6;

Publishing Information

Journal Title
Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment
Journal Volume
732
Journal Page Range
p. 52-56
ISSN
0168-9002
CODEN
NIMAER

Conference

Title
13. Vienna conference on instrumentation
Dates
11-15 Feb 2013
Place
Vienna (Austria)

Optional Information

Copyright
Copyright (c) 2013 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.