A facility for measurements of nuclear cross sections for fast neutron cancer therapy

A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within, e.g., fast neutron cancer therapy, is described. The central detection elements are three-detector telescopes consisting of two silicon detectors and a CsI crystal. Use of...

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Vydáno v:	Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Ročník 452; číslo 3; s. 484 - 504
Hlavní autoři:	Dangtip, S, Ataç, A, Bergenwall, B, Blomgren, J, Elmgren, K, Johansson, C, Klug, J, Olsson, N, Carlsson, G.Alm, Söderberg, J, Jonsson, O, Nilsson, L, Renberg, P.-U, Nadel-Turonski, P, Brun, C.Le, Lecolley, F.-R, Lecolley, J.-F, Varignon, C, Eudes, Ph, Haddad, F, Kerveno, M, Kirchner, T, Lebrun, C
Médium:	Journal Article
Jazyk:	angličtina
Vydáno:	Elsevier B.V 01.10.2000 Elsevier
Témata:	Biological Physics Carbon Cesium compounds Charged particle spectrometer array Computer software MEDICIN MEDICINE Neutron spectrometers Nuclear reactions Oncology Optical collimators Particle detectors Phosphors Physics Semiconducting silicon Telescopes Charged particle spectrometer array 29.40.Mc 25.40.−h Nuclear reactions 29.30.Ep 29.40.Wk charged particle spectrometer array HELIUM SPECTRA LIGHT CHARGED-PARTICLE PHOTODIODE READOUT DIFFERENTIAL INCLUSIVE HYDROGEN CSI(TL) SCINTILLATOR INDUCED SOFT ERRORS HEAVY-IONS KERMA FACTORS ENERGY-RANGE nuclear reactions SALIVARY-GLAND TUMORS
ISSN:	0168-9002, 1872-9576, 1872-9576
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Abstract	A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within, e.g., fast neutron cancer therapy, is described. The central detection elements are three-detector telescopes consisting of two silicon detectors and a CsI crystal. Use of Δ E–Δ E– E techniques allows good particle identification for p, d, t, 3He and alpha particles over an energy range from a few MeV up to 100 MeV. Active plastic scintillator collimators are used to define the telescope solid angle. Measurements can be performed using up to eight telescopes at 20° intervals simultaneously, thus covering a wide angular range. The performance of the equipment is illustrated using experimental data taken with a carbon target at E n=95 MeV. Distortions of the measured charged-particle spectra due to energy and particle losses in the target are corrected using a newly developed computer code. Results from such correction calculations are presented.
AbstractList	A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within, e.g., fast neutron cancer therapy, is described. The central detection elements are three-detector telescopes consisting of two silicon detectors and a CsI crystal. Use of ?E-?E-E techniques allows good particle identification for p, d, t, 3He and alpha particles over an energy range from a few MeV up to 100 MeV. Active plastic scintillator collimators are used to define the telescope solid angle. Measurements can be performed using up to eight telescopes at 20░ intervals simultaneously, thus covering a wide angular range. The performance of the equipment is illustrated using experimental data taken with a carbon target at En = 95 MeV. Distortions of the measured charged-particle spectra due to energy and particle losses in the target are corrected using a newly developed computer code. Results from such correction calculations are presented. A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within, e.g., fast neutron cancer therapy, is described. The central detection elements are three-detector telescopes consisting of two silicon detectors and a CsI crystal. Use of Δ E–Δ E– E techniques allows good particle identification for p, d, t, 3He and alpha particles over an energy range from a few MeV up to 100 MeV. Active plastic scintillator collimators are used to define the telescope solid angle. Measurements can be performed using up to eight telescopes at 20° intervals simultaneously, thus covering a wide angular range. The performance of the equipment is illustrated using experimental data taken with a carbon target at E n=95 MeV. Distortions of the measured charged-particle spectra due to energy and particle losses in the target are corrected using a newly developed computer code. Results from such correction calculations are presented. A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within. e.g.. fast neutron cancer therapy, is described. The central detection elements are three-detector telescopes consisting of two A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within, e.g., fast neutron cancer therapy, is described. The central detection elements are three-detector telescopes consisting of two silicon detectors and a CsI crystal. Use of Delta E- Delta E-E techniques allows good particle identification for p, d, t, super(3)He and alpha particles over an energy range from a few MeV up to 100 MeV. Active plastic scintillator collimators are used to define the telescope solid angle. Measurements can be performed using up to eight telescopes at 20 degree intervals simultaneously, thus covering a wide angular range. The performance of the equipment is illustrated using experimental data taken with a carbon target at E sub(n) identical with 95 MeV. Distortions of the measured charged-particle spectra due to energy and particle losses in the target are corrected using a newly developed computer code. Results from such correction calculations are presented.
Author	Johansson, C Nilsson, L Eudes, Ph Carlsson, G.Alm Varignon, C Lecolley, J.-F Elmgren, K Olsson, N Blomgren, J Kirchner, T Bergenwall, B Kerveno, M Ataç, A Jonsson, O Söderberg, J Nadel-Turonski, P Brun, C.Le Renberg, P.-U Dangtip, S Lecolley, F.-R Lebrun, C Haddad, F Klug, J
Author_xml	– sequence: 1 givenname: S surname: Dangtip fullname: Dangtip, S organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 2 givenname: A surname: Ataç fullname: Ataç, A organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 3 givenname: B surname: Bergenwall fullname: Bergenwall, B organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 4 givenname: J surname: Blomgren fullname: Blomgren, J organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 5 givenname: K surname: Elmgren fullname: Elmgren, K organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 6 givenname: C surname: Johansson fullname: Johansson, C organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 7 givenname: J surname: Klug fullname: Klug, J organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 8 givenname: N surname: Olsson fullname: Olsson, N email: nils.olsson@tsl.uu.se organization: Department of Neutron Research, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 9 givenname: G.Alm surname: Carlsson fullname: Carlsson, G.Alm organization: Department of Radiology and Radiation Physics, Linköping University, S-58185 Linköping, Sweden – sequence: 10 givenname: J surname: Söderberg fullname: Söderberg, J organization: Department of Radiology and Radiation Physics, Linköping University, S-58185 Linköping, Sweden – sequence: 11 givenname: O surname: Jonsson fullname: Jonsson, O organization: The Svedberg Laboratory, Uppsala University, Box 533, S-75121 Uppsala, Sweden – sequence: 12 givenname: L surname: Nilsson fullname: Nilsson, L organization: The Svedberg Laboratory, Uppsala University, Box 533, S-75121 Uppsala, Sweden – sequence: 13 givenname: P.-U surname: Renberg fullname: Renberg, P.-U organization: The Svedberg Laboratory, Uppsala University, Box 533, S-75121 Uppsala, Sweden – sequence: 14 givenname: P surname: Nadel-Turonski fullname: Nadel-Turonski, P organization: Department of Radiation Sciences, Uppsala University, Box 535, S-75121 Uppsala, Sweden – sequence: 15 givenname: C.Le surname: Brun fullname: Brun, C.Le organization: LPC, ISMRA et Université de Caen, CNRS/IN2P3, 14050 Caen Cedex, France – sequence: 16 givenname: F.-R surname: Lecolley fullname: Lecolley, F.-R organization: LPC, ISMRA et Université de Caen, CNRS/IN2P3, 14050 Caen Cedex, France – sequence: 17 givenname: J.-F surname: Lecolley fullname: Lecolley, J.-F organization: LPC, ISMRA et Université de Caen, CNRS/IN2P3, 14050 Caen Cedex, France – sequence: 18 givenname: C surname: Varignon fullname: Varignon, C organization: LPC, ISMRA et Université de Caen, CNRS/IN2P3, 14050 Caen Cedex, France – sequence: 19 givenname: Ph surname: Eudes fullname: Eudes, Ph organization: SUBATECH, Université de Nantes, CNRS/IN2P3, 44070 Nantes Cedex 03, France – sequence: 20 givenname: F surname: Haddad fullname: Haddad, F organization: SUBATECH, Université de Nantes, CNRS/IN2P3, 44070 Nantes Cedex 03, France – sequence: 21 givenname: M surname: Kerveno fullname: Kerveno, M organization: SUBATECH, Université de Nantes, CNRS/IN2P3, 44070 Nantes Cedex 03, France – sequence: 22 givenname: T surname: Kirchner fullname: Kirchner, T organization: SUBATECH, Université de Nantes, CNRS/IN2P3, 44070 Nantes Cedex 03, France – sequence: 23 givenname: C surname: Lebrun fullname: Lebrun, C organization: SUBATECH, Université de Nantes, CNRS/IN2P3, 44070 Nantes Cedex 03, France
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Keywords	Charged particle spectrometer array 29.40.Mc 25.40.−h Nuclear reactions 29.30.Ep 29.40.Wk charged particle spectrometer array HELIUM SPECTRA LIGHT CHARGED-PARTICLE PHOTODIODE READOUT DIFFERENTIAL INCLUSIVE HYDROGEN CSI(TL) SCINTILLATOR INDUCED SOFT ERRORS HEAVY-IONS KERMA FACTORS ENERGY-RANGE nuclear reactions SALIVARY-GLAND TUMORS
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Snippet	A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within, e.g., fast neutron cancer... A facility for measurements of neutron-induced double-differential light-ion production cross-sections, for application within. e.g.. fast neutron cancer...
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SubjectTerms	Biological Physics Carbon Cesium compounds Charged particle spectrometer array Computer software MEDICIN MEDICINE Neutron spectrometers Nuclear reactions Oncology Optical collimators Particle detectors Phosphors Physics Semiconducting silicon Telescopes
Title	A facility for measurements of nuclear cross sections for fast neutron cancer therapy
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