The silicon microstrip tracker for CMS View Full Text


Ontology type: schema:ScholarlyArticle     


Article Info

DATE

1999-11

AUTHORS

S. Albergo, M. Angarano, P. Azzi, E. Babucci, N. Bacchetta, A. Bader, G. Bagliesi, A. Basti, U. Biggeri, G. M. Bilei, D. Bisello, D. Boem i, F. Bosi, L. Borrello, C. Bozzi, S. Braibant, H. Breuker, M. Bruzzi, A. Buffini, S. Busoni, A. Candelori, A. Caner, R. Castaldi, A. Castro, E. Catacchini, B. Checcucci, P. Ciampolini, C. Civinini, D. Creanza, R. D’Alessandro, M. Da Rold, N. Dem aria, M. de Palma, R. Dell’Orso, R. Della Marina, S. Dutta, C. Eklund, L. Feld, L. Fiore, E. Focardi, M. French, K. Freudenreich, A. Frey, A. Fürtjes, A. Giassi, M. Giorgi, A. Giraldo, B. Glessing, W. H. Gu, G. Hall, R. Hammarstrom, T. Hebbeker, A. Honma, J. Hrubec, M. Huhtinen, A. Kam insky, V. Karimaki, St. Koenig, M. Kram m er, P. Lariccia, M. Lenzi, M. Loreti, K. Luebelsmeyer, W. Lustermann, P. Mättig, G. Maggi, M. Mannelli, G. Mantovani, A. Marchioro, C. Mariotti, G. Martignon, B. Mc Evoy, M. Meschini, A. Messineo, E. Migliore, S. My, A. Paccagnella, F. Palla, D. Pandoulas, A. Papi, G. Parrini, D. Passeri, M. Pieri, S. Piperov, R. Potenza, V. Radicci, F. Raffaelli, M. Raym ond, F. Rizzo, A. Santocchia, B. Schmitt, G. Selvaggi, L. Servoli, G. Sguazzoni, R. Siedling, L. Silvestris, A. Starodum ov, I. Stavitski, G. Stefanini, B. Surrow, P. Tempesta, G. Tonelli, A. Tricomi, T. Tuuva, C. Vannini, P. G. Verdini, G. Viertel, Z. Xie, Li Yahong, S. Watts, B. Wittmer

ABSTRACT

This paper describes the silicon microstrip tracker of the CMS experiment at the future LHC. The silicon tracker consists of a barrel part with 5 layers and two endcaps with 10 disks each. About 6500 modules will have to be built, each one carrying two daisy-chained silicon sensors and their front-end electronics. The modules have been designed to be as simple and robust as possible. Radiation damage in the silicon sensors is minimized by cooling the whole system down to -10°C. Safe operation after heavy irradiation will be possible due to the high-voltage capability of the sensors. We expect the sensors to have a signal-to-noise ratio of 10 at the end of 10years of LHC running, which still gives an efficiency of almost 100%. More... »

PAGES

1307-1316

Identifiers

URI

http://scigraph.springernature.com/pub.10.1007/bf03185596

DOI

http://dx.doi.org/10.1007/bf03185596

DIMENSIONS

https://app.dimensions.ai/details/publication/pub.1012394067


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