BibTex format
@inproceedings{Acharya:2021,
author = {Acharya, B and Alexandre, J and Beneš, P and Bergmann, B and Bevan, A and Billoud, T and Branzas, H and Burian, P and Campbell, M and Cecchini, S and Cho, YM and de, Montigny M and de, Roeck A and Ellis, JR and El, Sawy MMH and Fairbairn, M and Felea, D and Frank, M and Garvey, D and Hays, J and Hirt, AM and Janecek, J and Kalliokoski, M and Korzenev, A and Lacarrère, DH and Leroy, C and Levi, G and Lionti, A and Mánek, P and Maulik, A and Margiotta, A and Mauri, N and Mavromatos, NE and Meduna, L and Mermod, P and Millward, L and Mitsou, VA and Ostrovskiy, I and Ouimet, PP and Papavassiliou, J and Parker, B and Patrizii, L and Pavalas, GE and Pinfold, JL and Popa, LA and Popa, V and Pozzato, M and Pospíšil, S and Rajantie, A and de, Austri RR and Sahnoun, Z and Sakellariadou, M and Santra, A and Sarkar, S and Semenoff, G and Shaa, A and Sirri, G and Sliwa, K and Smolyanskiy, P and Soluk, R and Spurio, M and Staelens, M and Suk, M and Tenti, M and Tog},
title = {Timepix3 as a solid-state time-projection chamber in particle and nuclear physics},
year = {2021}
}
RIS format (EndNote, RefMan)
TY - CPAPER
AB - Timepix3 devices are hybrid pixel detectors developed within the Medipix3 collaboration at CERN providing a simultaneous measurement of energy (ToT) and time of arrival (ToA) in each of its 256 × 256 pixels (pixel pitch: 55 µm). The timestamp resolution below 2 ns allows a measurement of charge carrier drift times, so that particle trajectories can be reconstructed in 3D on a microscopic level (z-resolution: 30-60 µm). The 3D trajectory reconstruction methodology developed elsewhere is validated against simulated data providing ground truth information of the incident angles. The detector response functions and the achievable track angular resolutions are determined. For the first time, data taken with Timepix3 in the MoEDAL experiment are presented. After extracting singly charged minimum ionizing particle (MIP) tracks from the mixed radiation field using characteristic track features, their impact angles are evaluated. The directionality of the MIP radiation field is shown in elevation angle (?) versus azimuthal angle (?) maps, “unfolded” using the simulated detector responses to an omnidirectional radiation field.
AU - Acharya,B
AU - Alexandre,J
AU - Beneš,P
AU - Bergmann,B
AU - Bevan,A
AU - Billoud,T
AU - Branzas,H
AU - Burian,P
AU - Campbell,M
AU - Cecchini,S
AU - Cho,YM
AU - de,Montigny M
AU - de,Roeck A
AU - Ellis,JR
AU - El,Sawy MMH
AU - Fairbairn,M
AU - Felea,D
AU - Frank,M
AU - Garvey,D
AU - Hays,J
AU - Hirt,AM
AU - Janecek,J
AU - Kalliokoski,M
AU - Korzenev,A
AU - Lacarrère,DH
AU - Leroy,C
AU - Levi,G
AU - Lionti,A
AU - Mánek,P
AU - Maulik,A
AU - Margiotta,A
AU - Mauri,N
AU - Mavromatos,NE
AU - Meduna,L
AU - Mermod,P
AU - Millward,L
AU - Mitsou,VA
AU - Ostrovskiy,I
AU - Ouimet,PP
AU - Papavassiliou,J
AU - Parker,B
AU - Patrizii,L
AU - Pavalas,GE
AU - Pinfold,JL
AU - Popa,LA
AU - Popa,V
AU - Pozzato,M
AU - Pospíšil,S
AU - Rajantie,A
AU - de,Austri RR
AU - Sahnoun,Z
AU - Sakellariadou,M
AU - Santra,A
AU - Sarkar,S
AU - Semenoff,G
AU - Shaa,A
AU - Sirri,G
AU - Sliwa,K
AU - Smolyanskiy,P
AU - Soluk,R
AU - Spurio,M
AU - Staelens,M
AU - Suk,M
AU - Tenti,M
AU - Togo,V
AU - Tuszynski,JA
AU - Upreti,A
AU - Vento,V
AU - Vives,O
AU - Wall,A
AU - White,E
PY - 2021///
TI - Timepix3 as a solid-state time-projection chamber in particle and nuclear physics
ER -