Pre- and post-irradiation performance of FBK 3D silicon pixel detectors for CMS

Krzywda, A.; Alagöz, E.; Bubna, M.; Obertino, M. M.; Solano, A.; Arndt, K.; Uplegger, L.; Betta, G.-F. Dalla; Boscardin, M.; Ngadiuba, J.; Rivera, R.; Menasce, D.; Moroni, L.; Terzo, S.; Bortoletto, D.; Prosser, A.; Adreson, J.; Kwan, S.; Osipenkov, I.; Bolla, G.; Lei, C. M.; Shipsey, I. P. J.; Tan, P.; Tran, N. V.; Chramowicz, J.; Cumalat, J. P.; Perera, L.; Povoli, Marco; Mendicino, R.; Pereira, A. Vilela; Brosius, Richard; Kumar, Ashish; Wagner, S. R.; Jensen, F.; Bose, S. K.; Tentindo, S.

doi:10.1016/j.nima.2014.06.029

Cited by 3 publications

(3 citation statements)

References 23 publications

(23 reference statements)

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“…The detector hardware and control software is complemented by the Monicelli software, which provides to the users the reconstructed tracks necessary for their data analysis. The telescope has already been used by several experiments and, in particular, has been extensively used by the CMS forward pixel community to test sensor candidates for future CMS pixel upgrades [7][8][9][10][11][12][13][14][15].…”

Section: Discussionmentioning

confidence: 99%

The pixel tracking telescope at the Fermilab Test Beam Facility

Kwan

Lei

Menasce

et al. 2016

Nuclear Instruments and Methods in Physics Research Section A:

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An all silicon pixel telescope has been assembled and used at the Fermilab Test Beam Facility (FTBF) since 2009 to provide precise tracking information for different test beam experiments with a wide range of Detectors Under Test (DUTs) requiring high resolution measurement of the track impact point. The telescope is based on CMS pixel modules left over from the CMS forward pixel production. Eight planes are arranged to achieve a resolution of less than 8 μm on the 120 GeV proton beam transverse coordinate at the DUT position. In order to achieve such resolution with 100  150 μm 2 pixel cells, the planes were tilted to 25 degrees to maximize charge sharing between pixels. Crucial for obtaining this performance is the alignment software, called Monicelli, specifically designed and optimized for this system. This paper will describe the telescope hardware, the data acquisition system and the alignment software constituting this particle tracking system for test beam users.

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Section: Discussionmentioning

confidence: 99%

The pixel tracking telescope at the Fermilab Test Beam Facility

Kwan

Lei

Menasce

et al. 2016

Nuclear Instruments and Methods in Physics Research Section A:

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“…Uniform irradiation studies were performed for CMS/PPS PSI46 3D devices. Previous investigations [33,34] were limited by the old version of the analog PSI46 readout chip that was not radiation hard enough, but a preliminary analysis of recent studies with the new digital PSI46dig chip could demonstrate hit efficiencies of 98% (93%) after 1 (3) ×10 15 n eq /cm 2 with FBK 3D sensors with only one 3D junction column per pixel [32]. The performance is expected to improve with devices that include two junction columns per pixel.…”

Section: D Detectors In Forward Detectors (Afp and Pps)mentioning

confidence: 99%

Recent progress on 3D silicon detectors

Lange¹

2015

Proceedings of 24th International Workshop on Vertex Detectors — PoS(VERTEX2015)

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3D silicon detectors, in which the electrodes penetrate the sensor bulk perpendicular to the surface, have recently undergone a rapid development from R&D over industrialisation to their first installation in a real high-energy-physics experiment. Since June 2015, the ATLAS Insertable B-Layer is taking first collision data with 3D pixel detectors. At the same time, preparations are advancing to install 3D pixel detectors in forward trackers such as the ATLAS Forward Proton detector or the CMS-TOTEM Proton Precision Spectrometer. For those experiments, the main requirements are a slim edge and the ability to cope with non-uniform irradiation. Both have been shown to be fulfilled by 3D pixel detectors. For the High-Luminosity LHC pixel upgrades of the major experiments, 3D detectors are promising candidates for the innermost pixel layers to cope with harsh radiation environments up to fluences of 2 × 10 16 n eq /cm 2 thanks to their excellent radiation hardness at low operational voltages and power dissipation as well as moderate temperatures. This paper will give an overview on the recent developments of 3D detectors related to the projects mentioned above and the future plans.

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“…In terms of functional properties, remarkable performances have been demonstrated for the IBL 3D sensors: in particular, they have shown hit reconstruction efficiency >98% for 15º inclined tracks at 160 V bias after 5x10 15 n eq /cm 2 [9]. Very encouraging results have also been obtained from the characterization of 3D pixel prototypes compatible with the PSI46 read-out chip [22], [23].…”

Section: State Of the Artmentioning

confidence: 99%

3D Silicon Detectors

Betta¹

2015

Proceedings of INFN Workshop on Future Detectors for HL-LHC — PoS(IFD2014)

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Pre- and post-irradiation performance of FBK 3D silicon pixel detectors for CMS

Cited by 3 publications

References 23 publications

The pixel tracking telescope at the Fermilab Test Beam Facility

The pixel tracking telescope at the Fermilab Test Beam Facility

Recent progress on 3D silicon detectors

3D Silicon Detectors

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