The Bergen proton CT system

M. Aehle,J. Alme,G.G. Barnaföldi, T. Bodova, V. Borshchov,A. van den Brink, M. Chaar,V. Eikeland,G. Feofilov, C. Garth, N.R. Gauger,G. Genov, O. Grøttvik,H. Helstrup, S. Igolkin, R. Keidel,C. Kobdaj, T. Kortus, V. Leonhardt, S. Mehendale, R.N. Mulawade, O.H. Odland,G. O’Neill,G. Papp, T. Peitzmann, H.E.S. Pettersen,P. Piersimoni,M. Protsenko, M. Rauch,A. Ur Rehman, M. Richter, D. Röhrich, J. Santana, A. Schilling, J. Seco,A. Songmoolnak, J.R. Sølie,G. Tambave,I. Tymchuk, K. Ullaland, M. Varga-Köfaragó,L. Volz, B. Wagner,S. Wendzel,A. Wiebel, R. Xiao,S. Yang, H. Yokoyama, S. Zillien

Journal of Instrumentation(2023)

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Abstract
Abstract The Bergen proton Computed Tomography (pCT) is a prototype detector under construction. It aims to have the capability to track and measure ions’ energy deposition to minimize uncertainty in proton treatment planning. It is a high granularity digital tracking calorimeter, where the first two layers will act as tracking layers to obtain positional information of the incoming particle. The remainder of the detector will act as a calorimeter. Beam tests have been performed with multiple beams. These tests have shown that the ALPIDE chip sensor can measure the deposited energy, making it possible for the sensors to distinguish between the tracks in the Digital Tracking Calorimeter (DTC).
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Key words
Image reconstruction in medical imaging, Computerized Tomography (CT) and Computed Radiography (CR), Instrumentation for hadron therapy
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