Standard

The Bergen proton CT system. / Aehle, M.; Alme, J.; Barnaföldi, G.g.; Bodova, T.; Borshchov, V.; Van Den Brink, A.; Chaar, M.; Eikeland, V.; Feofilov, G.; Garth, C.; Gauger, N.r.; Genov, G.; Grøttvik, O.; Helstrup, H.; Igolkin, S.; Keidel, R.; Kobdaj, C.; Kortus, T.; Leonhardt, V.; Mehendale, S.; Mulawade, R.n.; Odland, O.h.; O’neill, G.; Papp, G.; Peitzmann, T.; Pettersen, H.e.s.; Piersimoni, P.; Protsenko, M.; Rauch, M.; Ur Rehman, A.; Richter, M.; Röhrich, D.; Santana, J.; Schilling, A.; Seco, J.; Songmoolnak, A.; Sølie, J.r.; Tambave, G.; Tymchuk, I.; Ullaland, K.; Varga-köfaragó, M.; Volz, L.; Wagner, B.; Wendzel, S.; Wiebel, A.; Xiao, R.; Yang, S.; Yokoyama, H.; Zillien, S.

в: Journal of Instrumentation, Том 18, № 02, C02051, 01.02.2023.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

Harvard

Aehle, M, Alme, J, Barnaföldi, GG, Bodova, T, Borshchov, V, Van Den Brink, A, Chaar, M, Eikeland, V, Feofilov, G, Garth, C, Gauger, NR, Genov, G, Grøttvik, O, Helstrup, H, Igolkin, S, Keidel, R, Kobdaj, C, Kortus, T, Leonhardt, V, Mehendale, S, Mulawade, RN, Odland, OH, O’neill, G, Papp, G, Peitzmann, T, Pettersen, HES, Piersimoni, P, Protsenko, M, Rauch, M, Ur Rehman, A, Richter, M, Röhrich, D, Santana, J, Schilling, A, Seco, J, Songmoolnak, A, Sølie, JR, Tambave, G, Tymchuk, I, Ullaland, K, Varga-köfaragó, M, Volz, L, Wagner, B, Wendzel, S, Wiebel, A, Xiao, R, Yang, S, Yokoyama, H & Zillien, S 2023, 'The Bergen proton CT system', Journal of Instrumentation, Том. 18, № 02, C02051. https://doi.org/10.1088/1748-0221/18/02/c02051

APA

Aehle, M., Alme, J., Barnaföldi, G. G., Bodova, T., Borshchov, V., Van Den Brink, A., Chaar, M., Eikeland, V., Feofilov, G., Garth, C., Gauger, N. R., Genov, G., Grøttvik, O., Helstrup, H., Igolkin, S., Keidel, R., Kobdaj, C., Kortus, T., Leonhardt, V., ... Zillien, S. (2023). The Bergen proton CT system. Journal of Instrumentation, 18(02), [C02051]. https://doi.org/10.1088/1748-0221/18/02/c02051

Vancouver

Aehle M, Alme J, Barnaföldi GG, Bodova T, Borshchov V, Van Den Brink A и пр. The Bergen proton CT system. Journal of Instrumentation. 2023 Февр. 1;18(02). C02051. https://doi.org/10.1088/1748-0221/18/02/c02051

Author

Aehle, M. ; Alme, J. ; Barnaföldi, G.g. ; Bodova, T. ; Borshchov, V. ; Van Den Brink, A. ; Chaar, M. ; Eikeland, V. ; Feofilov, G. ; Garth, C. ; Gauger, N.r. ; Genov, G. ; Grøttvik, O. ; Helstrup, H. ; Igolkin, S. ; Keidel, R. ; Kobdaj, C. ; Kortus, T. ; Leonhardt, V. ; Mehendale, S. ; Mulawade, R.n. ; Odland, O.h. ; O’neill, G. ; Papp, G. ; Peitzmann, T. ; Pettersen, H.e.s. ; Piersimoni, P. ; Protsenko, M. ; Rauch, M. ; Ur Rehman, A. ; Richter, M. ; Röhrich, D. ; Santana, J. ; Schilling, A. ; Seco, J. ; Songmoolnak, A. ; Sølie, J.r. ; Tambave, G. ; Tymchuk, I. ; Ullaland, K. ; Varga-köfaragó, M. ; Volz, L. ; Wagner, B. ; Wendzel, S. ; Wiebel, A. ; Xiao, R. ; Yang, S. ; Yokoyama, H. ; Zillien, S. / The Bergen proton CT system. в: Journal of Instrumentation. 2023 ; Том 18, № 02.

BibTeX

@article{815ecc3159424b528ca32adc2fb6cca6,
title = "The Bergen proton CT system",
abstract = "The Bergen proton Computed Tomography (pCT) is a prototype detector under construction. It aims to have the capability to track and measure ions{\textquoteright} 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).",
keywords = "Computerized Tomography (CT) and Computed Radiography (CR), Image reconstruction in medical imaging, Instrumentation for hadron therapy",
author = "M. Aehle and J. Alme and G.g. Barnaf{\"o}ldi and T. Bodova and V. Borshchov and {Van Den Brink}, A. and M. Chaar and V. Eikeland and G. Feofilov and C. Garth and N.r. Gauger and G. Genov and O. Gr{\o}ttvik and H. Helstrup and S. Igolkin and R. Keidel and C. Kobdaj and T. Kortus and V. Leonhardt and S. Mehendale and R.n. Mulawade and O.h. Odland and G. O{\textquoteright}neill and G. Papp and T. Peitzmann and H.e.s. Pettersen and P. Piersimoni and M. Protsenko and M. Rauch and {Ur Rehman}, A. and M. Richter and D. R{\"o}hrich and J. Santana and A. Schilling and J. Seco and A. Songmoolnak and J.r. S{\o}lie and G. Tambave and I. Tymchuk and K. Ullaland and M. Varga-k{\"o}farag{\'o} and L. Volz and B. Wagner and S. Wendzel and A. Wiebel and R. Xiao and S. Yang and H. Yokoyama and S. Zillien",
year = "2023",
month = feb,
day = "1",
doi = "10.1088/1748-0221/18/02/c02051",
language = "English",
volume = "18",
journal = "Journal of Instrumentation",
issn = "1748-0221",
publisher = "IOP Publishing Ltd.",
number = "02",

}

RIS

TY - JOUR

T1 - The Bergen proton CT system

AU - Aehle, M.

AU - Alme, J.

AU - Barnaföldi, G.g.

AU - Bodova, T.

AU - Borshchov, V.

AU - Van Den Brink, A.

AU - Chaar, M.

AU - Eikeland, V.

AU - Feofilov, G.

AU - Garth, C.

AU - Gauger, N.r.

AU - Genov, G.

AU - Grøttvik, O.

AU - Helstrup, H.

AU - Igolkin, S.

AU - Keidel, R.

AU - Kobdaj, C.

AU - Kortus, T.

AU - Leonhardt, V.

AU - Mehendale, S.

AU - Mulawade, R.n.

AU - Odland, O.h.

AU - O’neill, G.

AU - Papp, G.

AU - Peitzmann, T.

AU - Pettersen, H.e.s.

AU - Piersimoni, P.

AU - Protsenko, M.

AU - Rauch, M.

AU - Ur Rehman, A.

AU - Richter, M.

AU - Röhrich, D.

AU - Santana, J.

AU - Schilling, A.

AU - Seco, J.

AU - Songmoolnak, A.

AU - Sølie, J.r.

AU - Tambave, G.

AU - Tymchuk, I.

AU - Ullaland, K.

AU - Varga-köfaragó, M.

AU - Volz, L.

AU - Wagner, B.

AU - Wendzel, S.

AU - Wiebel, A.

AU - Xiao, R.

AU - Yang, S.

AU - Yokoyama, H.

AU - Zillien, S.

PY - 2023/2/1

Y1 - 2023/2/1

N2 - 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).

AB - 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).

KW - Computerized Tomography (CT) and Computed Radiography (CR)

KW - Image reconstruction in medical imaging

KW - Instrumentation for hadron therapy

UR - https://www.mendeley.com/catalogue/48bcf029-986a-3b66-9d92-4ee36fb9845d/

UR - https://www.mendeley.com/catalogue/48bcf029-986a-3b66-9d92-4ee36fb9845d/

U2 - 10.1088/1748-0221/18/02/c02051

DO - 10.1088/1748-0221/18/02/c02051

M3 - Article

VL - 18

JO - Journal of Instrumentation

JF - Journal of Instrumentation

SN - 1748-0221

IS - 02

M1 - C02051

ER -

ID: 106597674