|
1.
|
The ABC130 barrel module prototyping programme for the ATLAS strip tracker
/ ATLAS Collaboration
For the Phase-II Upgrade of the ATLAS Detector, its Inner Detector, consisting of silicon pixel, silicon strip and transition radiation sub-detectors, will be replaced with an all new 100 % silicon tracker, composed of a pixel tracker at inner radii and a strip tracker at outer radii. The future ATLAS strip tracker will include 11,000 silicon sensor modules in the central region (barrel) and 7,000 modules in the forward region (end-caps), which are foreseen to be constructed over a period of 3.5 years. [...]
arXiv:2009.03197.-
2020-09-03 - 82 p.
- Published in : JINST 15 (2020) P09004
Fulltext: PDF;
|
|
|
2.
|
Proprieties of FBK UFSDs after neutron and proton irradiation up to $6*10^{15}$ neq/cm$^2$
/ Mazza, S.M. (UC, Santa Cruz, Inst. Part. Phys.) ; Estrada, E. (UC, Santa Cruz, Inst. Part. Phys.) ; Galloway, Z. (UC, Santa Cruz, Inst. Part. Phys.) ; Gee, C. (UC, Santa Cruz, Inst. Part. Phys.) ; Goto, A. (UC, Santa Cruz, Inst. Part. Phys.) ; Luce, Z. (UC, Santa Cruz, Inst. Part. Phys.) ; McKinney-Martinez, F. (UC, Santa Cruz, Inst. Part. Phys.) ; Rodriguez, R. (UC, Santa Cruz, Inst. Part. Phys.) ; Sadrozinski, H.F.W. (UC, Santa Cruz, Inst. Part. Phys.) ; Seiden, A. (UC, Santa Cruz, Inst. Part. Phys.) et al.
The properties of 60-{\mu}m thick Ultra-Fast Silicon Detectors (UFSD) detectors manufactured by Fondazione Bruno Kessler (FBK), Trento (Italy) were tested before and after irradiation with minimum ionizing particles (MIPs) from a 90Sr \b{eta}-source . This FBK production, called UFSD2, has UFSDs with gain layer made of Boron, Boron low-diffusion, Gallium, Carbonated Boron and Carbonated. [...]
arXiv:1804.05449.-
2020-04-30 - 13 p.
- Published in : JINST 15 (2020) T04008
Fulltext: PDF;
|
|
|
3.
|
Comparison of 35 and 50 ${\mu}$m thin HPK UFSD after neutron irradiation up to $6•10^15$ $neq/cm^2$
/ Zhao, Y. (UC, Santa Cruz, Inst. Part. Phys.) ; Cartiglia, N. (UC, Santa Cruz, Inst. Part. Phys.) ; Estrada, E. (UC, Santa Cruz, Inst. Part. Phys.) ; Galloway, Z. (UC, Santa Cruz, Inst. Part. Phys.) ; Gee, C. (UC, Santa Cruz, Inst. Part. Phys.) ; Goto, A. (UC, Santa Cruz, Inst. Part. Phys.) ; Luce, Z. (UC, Santa Cruz, Inst. Part. Phys.) ; Mazza, S.M. (UC, Santa Cruz, Inst. Part. Phys.) ; Mckinney-Martinez, F. (UC, Santa Cruz, Inst. Part. Phys.) ; Rodriguez, R. (UC, Santa Cruz, Inst. Part. Phys.) et al.
We report results from the testing of 35 {\mu}m thick Ultra-Fast Silicon Detectors (UFSD produced by Hamamatsu Photonics (HPK), Japan and the comparison of these new results to data reported before on 50 {\mu}m thick UFSD produced by HPK. The 35 {\mu}m thick sensors were irradiated with neutrons to fluences of 0, 1*10^14, 1*10^15, 3*10^15, 6*10^15 neq/cm^2. [...]
arXiv:1803.02690.-
2019-04-21 - 7 p.
- Published in : Nucl. Instrum. Methods Phys. Res., A 924 (2019) 387-393
Fulltext: arXiv:1803.02690 - PDF; 1803.02690 - PDF;
In : 11th International "Hiroshima" Symposium on the Development and Application of Semiconductor Tracking Detectors (HSTD11) in conjunction with 2nd Workshop on SOI Pixel Detectors (SOIPIX2017) at OIST, Okinawa, Japan, Okinawa, Japan, 10 - 15 Dec 2017, pp.387-393
|
|
|
4.
|
Beam test measurements of Low Gain Avalanche Detector single pads and arrays for the ATLAS High Granularity Timing Detector
/ Allaire, C. (Orsay, LAL) ; Benitez, J. (U. Iowa, Iowa City) ; Bomben, M. (Paris U., VI-VII) ; Calderini, G. (Paris U., VI-VII) ; Carulla, M. (Barcelona, Inst. Microelectron.) ; Cavallaro, E. (Barcelona, IFAE) ; Falou, A. (Orsay, LAL) ; Flores, D. (Barcelona, Inst. Microelectron.) ; Freeman, P. (UC, Santa Cruz, Inst. Part. Phys.) ; Galloway, Z. (UC, Santa Cruz, Inst. Part. Phys.) et al.
For the high luminosity upgrade of the LHC at CERN, ATLAS is considering the addition of a High Granularity Timing Detector (HGTD) in front of the end cap and forward calorimeters at |z| = 3.5 m and covering the region 2.4 < |{\eta}| < 4 to help reducing the effect of pile-up. The chosen sensors are arrays of 50 {\mu}m thin Low Gain Avalanche Detectors (LGAD). [...]
arXiv:1804.00622.-
2018-06-20 - 28 p.
- Published in : JINST 13 (2018) P06017
Fulltext: Allaire_2018_J._Inst._13_P06017 - PDF; 1804.00622 - PDF; arXiv:1804.00622 - PDF; Fulltext from Publisher: PDF;
|
|
|
5.
|
Beam test results of a 16 ps timing system based on ultra-fast silicon detectors
/ Cartiglia, N. (INFN, Turin) ; Staiano, A. (INFN, Turin) ; Sola, V. (INFN, Turin) ; Arcidiacono, R. (Turin U., Alessandria ; INFN, Turin) ; Cirio, R. (Turin U. ; INFN, Turin) ; Cenna, F. (Turin U. ; INFN, Turin) ; Ferrero, M. (Turin U. ; INFN, Turin) ; Monaco, V. (Turin U. ; INFN, Turin) ; Mulargia, R. (Turin U. ; INFN, Turin) ; Obertino, M. (Turin U. ; INFN, Turin) et al.
In this paper we report on the timing resolution of the first production of 50 micro-meter thick Ultra-Fast Silicon Detectors (UFSD) as obtained in a beam test with pions of 180 GeV/c momentum. UFSD are based on the Low-Gain Avalanche Detectors (LGAD) design, employing n-on-p silicon sensors with internal charge multiplication due to the presence of a thin, low-resistivity diffusion layer below the junction. [...]
arXiv:1608.08681.-
2017-04-01 - 6 p.
- Published in : Nucl. Instrum. Methods Phys. Res., A 850 (2017) 83-88
Fulltext: 10.1016_j.nima.2017.01.021 - PDF; arXiv:1608.08681_2 - PDF; Preprint: PDF; External link: Preprint
|
|
alert email
lub zaprenumeruj 
RSS feed.