With the planned upgrade of the LHC to High-Luminosity-LHC, the general purpose experiments ATLAS and CMS are planning to upgrade their innermost tracking layers with more radiation tolerant technologies. Chemical Vapor Deposition CVD diamond is one such technology. CVD diamond sensors are an established technology as beam condition monitors in the highest radiation areas of all LHC experiments. The RD42-collaboration at CERN is leading the effort to use CVD diamond as a material for tracking detectors operating in extreme radiation environments. An overview of the latest developments from RD42 is presented including the present status of diamond sensor production, a study of pulse height dependencies on incident particle flux and the development of 3D diamond sensors.

Diamond sensors for future high energy experiments

FORNERIS, JACOPO;LO GIUDICE, Alessandro;OLIVERO, Paolo;PICOLLO, FEDERICO;RE, ALESSANDRO;VITTONE, Ettore;
2016-01-01

Abstract

With the planned upgrade of the LHC to High-Luminosity-LHC, the general purpose experiments ATLAS and CMS are planning to upgrade their innermost tracking layers with more radiation tolerant technologies. Chemical Vapor Deposition CVD diamond is one such technology. CVD diamond sensors are an established technology as beam condition monitors in the highest radiation areas of all LHC experiments. The RD42-collaboration at CERN is leading the effort to use CVD diamond as a material for tracking detectors operating in extreme radiation environments. An overview of the latest developments from RD42 is presented including the present status of diamond sensor production, a study of pulse height dependencies on incident particle flux and the development of 3D diamond sensors.
2016
831
370
377
http://www.sciencedirect.com/science/article/pii/S0168900216300560
3D sensors; Charge collection; CVD diamond; Diamond particle detector; Particle physics; Radiation hardness; Instrumentation; Nuclear and High Energy Physics
M. Artuso; F. Bachmair; L. Bani; M. Bartosik; J. Beacham; V. Bellini; V. Belyaev; B. Bentele; E. Berdermann; P. Bergonzo; A. Bes; J-M. Brom; M. Bruzzi; M. Cerv; C. Chau; G. Chiodini; D. Chren; V. Cindro; G. Claus; J. Collot; S. Costa; J. Cumalat; A. Dabrowski; R. D'Aessandro; W. de Boer; B. Dehning; D. Dobos; C. Dorfer; M. Dunser; V. Eremin; R. Eusebi; G. Forcolin; J. Forneris; H. Frais-Kolbl; K.K. Gan; M. Gastal; M. Goffe; J. Goldstein; A. Golubev; L. Gonella; A. Gorisek; L. Graber; E. Grigoriev; J. Grosse-Knetter; B. Gui; M. Guthoff; I. Haughton; D. Hidas; D. Hits; M. Hoeferkamp; T. Hofmann; J. Hosslet; J-Y. Hostachy; F. Hugging; H. Jansen; J. Janssen; H. Kagan; K. Kanxheri; G. Kasieczka; R. Kass; F. Kassel; M. Kis; G. Kramberger; S. Kuleshov; A. Lacoste; S. Lagomarsino; A. Lo Giudice; C. Maazouzi; I. Mandic; C. Mathieu; N. McFadden; G. McGoldrick; M. Menichelli; M. Mikuz; A. Morozzi; J. Moss; R. Mountain; S. Murphy; A. Oh; P. Olivero; G. Parrini; D. Passeri; M. Pauluzzi; H. Pernegger; R. Perrino; F. Picollo; M. Pomorski; R. Potenza; A. Quadt; A. Re; G. Riley; S. Roe; M. Sapinski; M. Scaringella; S. Schnetzer; T. Schreiner; S. Sciortino; A. Scorzoni; S. Seidel; L. Servoli; A. Sfyrla; G. Shimchuk; D.S. Smith; B. Sopko; V. Sopko; S. Spagnolo; S. Spanier; K. Stenson; R. Stone; C. Sutera; A. Taylor; M. Traeger; D. Tromson; W. Trischuk; C. Tuve; L. Uplegger; J. Velthuis; N. Venturi; E. Vittone; S. Wagner; R. Wallny; J. C. Wang; P. Weilhammer; J. Weingarten; C. Weiss; T. Wengler; N. Wermes; M. Yamouni; M. Zavrtanik
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/1589413
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