Cargando…

Radiation hardness studies of AMS HV-CMOS 350 nm prototype chip HVStripV1

CMOS active pixel sensors are being investigated for their potential use in the ATLAS inner tracker upgrade at the HL-LHC. The new inner tracker will have to handle a significant increase in luminosity while maintaining a sufficient signal-to-noise ratio and pulse shaping times. This paper focuses o...

Descripción completa

Detalles Bibliográficos
Autores principales: Kanisauskas, K, Affolder, A, Arndt, K, Bates, R, Benoit, M, Bello, F Di, Blue, A, Bortoletto, D, Buckland, M, Buttar, C, Caragiulo, P, Das, D, Dopke, J, Dragone, A, Ehrler, F, Fadeyev, V, Galloway, Z, Grabas, H, Gregor, I M, Grenier, P, Grillo, A, Hiti, B, Hoeferkamp, M, Hommels, L B A, Huffman, B T, John, J, Kenney, C, Kramberger, J, Liang, Z, Mandic, I, Maneuski, D, Martinez-Mckinney, F, MacMahon, S, Meng, L, Mikuž, M, Muenstermann, D, Nickerson, R, Peric, I, Phillips, P, Plackett, R, Rubbo, F, Segal, J, Seidel, S, Seiden, A, Shipsey, I, Song, W, Staniztki, M, Su, D, Tamma, C, Turchetta, R, Vigani, L, Volk, J, Wang, R, Warren, M, Wilson, F, Worm, S, Xiu, Q, Zhang, J, Zhu, H
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1748-0221/12/02/P02010
http://cds.cern.ch/record/2275299
Descripción
Sumario:CMOS active pixel sensors are being investigated for their potential use in the ATLAS inner tracker upgrade at the HL-LHC. The new inner tracker will have to handle a significant increase in luminosity while maintaining a sufficient signal-to-noise ratio and pulse shaping times. This paper focuses on the prototype chip 'HVStripV1' (manufactured in the AMS HV-CMOS 350nm process) characterization before and after irradiation up to fluence levels expected for the strip region in the HL-LHC environment. The results indicate an increase of depletion region after irradiation for the same bias voltage by a factor of ≈2.4 and ≈2.8 for two active pixels on the test chip. There was also a notable increase in noise levels from $85 e^−$ to $386 e^−$ and from $75 e^−$ to $277 e^−$ for the corresponding pixels.