ATLAS pixel detector electronics and sensors

Aad, G.; Ackers, M.; Alberti, Fabrizio; Aleppo, M.; Alimonti, G.; Alonso, J.; Anderssen, E.; Andreani, A.; Andreazza, A.; Arguin, J-F.; Arms, K.; Barberis, D.; Barbero, M.; Bazalova, M.; Beccherle, R.; Becks, K.H.; Behera, P. K.; Bellina, F.; Beringer, J.; Bernardet, K.; Biesiada, J.; Blanquart, L.; Boek, J.; Boyd, G.; Breugnon, P.; Buchholz, P.; Butler, B.; Caccia, M.; Capsoni, A.; Caso, C.; Cauz, D.; Cepeda, Mario; Cereseto, R.; Cervetto, M.; Chu, M. L.; Citterio, M.; Clémens, J. C.; Coadou, Y.; Cobal, M.; Coccaro, A.; Coelli, S.; Correard, S.; Cristinziani, M.; Cuneo, S.; D’Auria, S.; Dameri, M.; Darbo, G.; Dardin, S.; Lotto, B. De; Sanctis, U. De; Regie, J. De Vivie De B.; Papa, C. Del; Delpierre, P.; Girolamo, B. Di; Dietsche, W.; Djama, F.; Dobos, D.; Donegà, M.; Dopke, J.; Einsweiler, K.; Eyring, A.; Fasching, D.; Feligioni, L.; Ferguson, D.; Fernando, W.; Fischer, P.; Fisher, M.; Flick, T.; Gagliardi, G.; Galyaev, E.; Gan, K. K.; Garcia-Sciveres, M.; Garelli, N.; Gariano, G.; Gaycken, G.; Gemme, C.; Gerlach, P.; Gilchriese, M.; Giordani, M. P.; Giugni, D.; Glitza, K. W.; Gößling, C.; Golling, T.; Goozen, F.; Gorelov, I.; Gorfine, G.; Grah, C.; Gray, H. M.; Gregor, I. M.; Große-Knetter, J.; Grybel, K.; Gutiérrez, P.; Hallewell, G. D.; Hartman, Nicole Michelle; Havránek, M.; Heinemann, B.; Henß, T.; Hoeferkamp, M. R.; Hoffmann, D.; Holder, M.; Honerbach, W.; Horn, C.; Hou, S.; Huang, G. S.; Huegging, F.; Hughes, E. W.; Ibragimov, I.; Ilyashenko, I.; Imhaeuser, M.; Izen, J. M.; Jackson, J.; Jana, D. K.; Jared, R. C.; Jež, P.; Johnson, Thomas A.; Joseph, J.; Kagan, H.; Karagounis, M.; Kass, R.; Keil, M.; Kersten, S.; Kind, P.; Klaiber-Lodewigs, J.; Klingbeil, Lasse; Klingenberg, R.; Korn, A.; Kostyukhin, V. V.; Kostyukhina, I; Krasel, O.; Krüger, H.; Krueger, K.; Kudłaty, J.; Kühl, T.; Kvasnicka, O.; Lantzsch, K.; Lari, T.; Latorre, S.; Lee, S C; Lenz, T.; Lenzen, G.; Lepidis, J.; Levêque, J.; Leyton, M.; Mateos, D. Lopez; Loureiro, K. F.; Lüke, D.; Luisa, L.; Lys, J.; Madaras, R. J.; Mättig, P.; Manca, Fabio; Mandelli, E.; Marčišovský, M.; Marshall, Z.; Martı́nez, G.; Masetti, L.; Maß, M.; Mathes, M.; McKay, R.; Meddeler, G.; Meera-Lebbai, R.; Meroni, C.; Metcalfe, J.; Meyer, W. T.; Miller, D. W.; Miller, W.; Montesano, S.; Monti, M.; Morettini, P.; Moss, J.; Mouthuy, T.; Nechaeva, P. Y.; Ockenfels, W.; Odino, G. A.; Olcese, M.; Osculati, B.; Parodi, F.; Pekedis, Ahmet; Perez, K.; Perić, I.; Pizzorno, C.; Popule, J.; Post, Rodney; Ragusa, F.; Rahimi, A. M.; Raith, B.; Rajek, S.; Reeves, K.; Reisinger, I.; Richardson, J. D.; Rosenberg, E. I.; Rossi, L. P.; Rottländer, I.; Rovani, A.; Rozanov, A.; Runólfsson, Ö.; Ruscino, E.; Saavedra, A. F.; Sabatini, F.; Saleem, M.; Sandvoss, S.; Sanny, B.; Santi, L.; Scherzer, M. I.; Schiavi, C.; Schreiner, A.; Schultes, J.; Schwartzman, A.; Seibert, R.; Seidel, S. C.; Severini, H.; Shanava, S; Šı́cho, P.; Skubic, P.; Smith, A. C.; Smith, D. S.; Snow, J.; Stahl, T.; Stockmanns, T.; Strandberg, S.; Strauss, M.; Ta, D.; Tegenfeldt, F.; Teng, P. K.; Ter-Antonyan, R.; Thadome, J.; Tic, T.; Tomášek, L.; Tomášek, M.; Tomasi, F. De; Toms, K.; Tran, C.; Treis, J.; Triplett, N.; Troncon, C.; Vacavant, L.; Vahsen, S.; Valenta, J.; Vegni, G.; Vernocchi, F.; Vigeolas, E.; Virzi, J.; Viscione, E.; Vrba, V.; Walbersloh, J.; Walkowiak, W.; Weber, J.; Weber, Thorsten; Weingarten, J.; Weldon, C; Wermes, N.; Werthenbach, U.; Wirth, J.; Witharm, R.; Witt, Bernd; Wittgen, M.; Wuestenfeld, J.; Wunstorf, R.; Wyckoff, J.M.; Yao, W-M.; Young, C. C.; Zaidan, R.; Zdrazil, M.; Zetti, F.; Zhong, J.; Ziółkowski, M.; Zizka, G.; Zoeller, M.

doi:10.1088/1748-0221/3/07/p07007

Cited by 579 publications

(322 citation statements)

References 65 publications

(94 reference statements)

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“…The FE-I4 pixel array geometry is derived from that of the ATLAS pixel detector FE-I3 readout chip [6], wherein pixels are arranged in column pairs and power is segregated on vertical bands alternating between analog and digital. However, the readout architecture of FE-I4 is very different [7].…”

Section: Architecturementioning

confidence: 99%

The FE-I4 pixel readout integrated circuit

Garcia-Sciveres

Arutinov

Barbero

et al. 2011

Nuclear Instruments and Methods in Physics Research Section A:

273

243

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A new pixel readout integrated circuit denominated FE-I4 is being designed to meet the requirements of ATLAS experiment upgrades. It will be the largest readout IC produced to date for particle physics applications, filling the maximum allowed reticle area. This will significantly reduce the cost of future hybrid pixel detectors. In addition, FE-I4 will have smaller pixels and higher rate capability than the present generation of LHC pixel detectors. Design features are described along with simulation and test results, including low power and high rate readout architecture, mixed signal design strategy, and yield hardening.

show abstract

Section: Architecturementioning

confidence: 99%

The FE-I4 pixel readout integrated circuit

Garcia-Sciveres

Arutinov

Barbero

et al. 2011

Nuclear Instruments and Methods in Physics Research Section A:

273

243

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show abstract

“…The limitations of the current ATLAS pixel Front-End FE-I3 [2] -in particular for what concerns radiation hardness and its ability to cope with high hit rates-have been realized a few years ago [3] and have led to the development of a new IC series in a smaller feature size, the FE-I4. With respect to previous Front-End generations, the FE-I4 shows an increased tolerance to radiation which mainly comes from using only the thinner gate oxide transistors which are offered in the 130 nm CMOS process.…”

Section: The Fe-i4 Project and The Atlas Pixel Upgradesmentioning

confidence: 99%

FE-I4 pixel readout chip and IBL module

Barbero

Hemperek²,

Zivkovic³

et al. 2012

Proceedings of the 20th Anniversary International Workshop on Vertex Detectors — PoS(Vertex 2011)

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FE-I4 is the new ATLAS pixel readout chip for the upgraded ATLAS pixel detector. Designed in a CMOS 130 nm feature size process, the IC is able to withstand higher radiation levels compared to the present generation of ATLAS pixel Front-End FE-I3, and can also cope with higher hit rate. It is thus suitable for intermediate radii pixel detector layers in the High Luminosity LHC environment, but also for the inserted layer at 3.3 cm known as the "Insertable B-Layer" project (IBL), at a shorter timescale. In this paper, an introduction to the FE-I4 will be given, focusing on test results from the first full size FE-I4A prototype which has been available since fall 2010. The IBL project will be introduced, with particular emphasis on the FE-I4-based module concept.

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“…The innermost sub-system is called the Pixel detector [51,52]. This component has three layers in the barrel and three layers in each end cap, providing uniform coverage in φ for |η| < 2.5.…”

Section: The Atlas Detectormentioning

confidence: 99%

Search for Dark Matter Produced in Association with a Higgs Boson Decaying to Two Bottom Quarks at ATLAS

Cheng

2017

Springer Theses

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ATLAS pixel detector electronics and sensors

Cited by 579 publications

References 65 publications

The FE-I4 pixel readout integrated circuit

The FE-I4 pixel readout integrated circuit

FE-I4 pixel readout chip and IBL module

Search for Dark Matter Produced in Association with a Higgs Boson Decaying to Two Bottom Quarks at ATLAS

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