Charge-collection properties of irradiated depleted CMOS pixel test structures

被引:11
|
作者
Mandic, I [1 ]
Cindro, V [1 ]
Gorisek, A. [1 ]
Hiti, B. [1 ]
Kramberger, G. [1 ]
Zavrtanik, M. [1 ]
Mikuz, M. [1 ,2 ]
Hemperek, T. [3 ]
机构
[1] Jozef Stefan Inst, Jamova 39, Ljubljana, Slovenia
[2] Univ Ljubljana, Fac Math & Phys, Jadranska 19, Ljubljana, Slovenia
[3] Univ Bonn, Phys Inst, Nussallee 12, D-53115 Bonn, Germany
关键词
Particle-tracking detectors (Solid-state detectors); Radiation-hard detectors; Si microstrip and pad detectors; Solid-state detectors; !text type='JS']JS[!/text]I TRIGA REACTOR; SILICON DETECTORS; COMPUTATIONAL ANALYSIS; RADIATION-DAMAGE; P-TYPE; TECHNOLOGY; FACILITIES; UPGRADE;
D O I
10.1016/j.nima.2018.06.062
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
The edge transient-current technique (Edge-TCT) and charge-collection measurements with passive test structures made with the LFoundry 150-nm CMOS process on a p-type substrate with an initial resistivity of over 3 k Omega cm are presented. The measurements were made before and after irradiation with reactor neutrons up to 2.10(15) n(eq)/cm(2). Two sets of devices were investigated: unthinned (700 mu m) with the substrate biased through the implant on top and thinned (200 mu m) with a processed and metallised backplane. The depletion depth was estimated with the Edge-TCT and the collected charge was measured with a(90)Sr source using an external amplifier having a 25-ns shaping time. The depletion depth for a given bias voltage decreased with the increasing neutron fluence, but it was still larger than 70 mu m at 250 V after the highest fluence. After irradiation a much higher collected charge was measured for the thinned detectors with a processed backplane compared to the unthinned devices, although the same or an even larger depletion depth was measured in the unthinned devices. The most probable value of the collected charge of over 5000 electrons was measured with a thinned device also after irradiation to 2.10(15) n(eq)/cm(2). This is sufficient to ensure the successful operation of these detectors at the outer layer of the pixel detector in the ATLAS experiment at the upgraded HL-LHC.
引用
收藏
页码:126 / 133
页数:8
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