Literature DB >> 20821107

Nuclear collision processes around the Bragg peak in proton therapy.

Yuka Matsuzaki1, Hiroyuki Date, Kenneth Lee Sutherland, Yoshiaki Kiyanagi.   

Abstract

In the physical processes of proton interaction in bio-materials, most of the proton energy is transferred to electrons. Ionization and excitation occur most frequently around the Bragg peak region, where nuclear reactions also exist. In this study, we investigated the processes of energy deposition by considering interactions including the nuclear reactions between protons and water molecules by a Monte Carlo simulation for proton therapy. We estimated the number of particles produced by a variety of nuclear reactions, and we focused on the interaction in the low-energy region (below 1 MeV). Furthermore, we considered the charge-changing processes in the low-energy region (less than a few hundred keV). Finally, we evaluated the total dose and the contribution of primary protons and secondary particles through nuclear reactions to the absorbed dose. The results showed that the protons generate numerous neutrons via nuclear reactions. Particularly, neutrons with relatively low energies produce recoil protons by elastic collisions with the hydrogen atoms. Around the Bragg peak, low-energy primary protons (slowed-down protons) are prevalent, whereas recoil (secondary) protons gradually become dominant behind the distal falloff region of the Bragg peak. Therefore, around the Bragg peak, the main contribution to the absorbed dose is that of the primary protons (from 80 to 90%), whereas secondary protons created by primary proton-induced reactions contribute to the dose from 20 to 5%. Behind the distal endpoint of the Bragg peak, the absorbed dose is mainly due to the protons produced by (1)H(n, p), and the contribution of these is about 70%.

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Year:  2009        PMID: 20821107     DOI: 10.1007/s12194-009-0081-2

Source DB:  PubMed          Journal:  Radiol Phys Technol        ISSN: 1865-0333


  5 in total

1.  Nuclear interactions in proton therapy: dose and relative biological effect distributions originating from primary and secondary particles.

Authors:  H Paganetti
Journal:  Phys Med Biol       Date:  2002-03-07       Impact factor: 3.609

2.  Proton dose monitoring with PET: quantitative studies in Lucite.

Authors:  U Oelfke; G K Lam; M S Atkins
Journal:  Phys Med Biol       Date:  1996-01       Impact factor: 3.609

3.  Secondary neutron dose during proton therapy using spot scanning.

Authors:  Uwe Schneider; Stefano Agosteo; Eros Pedroni; Jürgen Besserer
Journal:  Int J Radiat Oncol Biol Phys       Date:  2002-05-01       Impact factor: 7.038

4.  Distributions of beta+ decayed nuclei generated in the CH2 and H2O targets by the target nuclear fragment reaction using therapeutic MONO and SOBP proton beam.

Authors:  Teiji Nishio; Takashi Sato; Hideaki Kitamura; Koji Murakami; Takashi Ogino
Journal:  Med Phys       Date:  2005-04       Impact factor: 4.071

5.  A Monte Carlo dose calculation algorithm for proton therapy.

Authors:  Matthias Fippel; Martin Soukup
Journal:  Med Phys       Date:  2004-08       Impact factor: 4.071

  5 in total
  2 in total

1.  Impact of ATM and DNA-PK Inhibition on Gene Expression and Individual Response of Human Lymphocytes to Mixed Beams of Alpha Particles and X-Rays.

Authors:  Lei Cheng; Beata Brzozowska-Wardecka; Halina Lisowska; Andrzej Wojcik; Lovisa Lundholm
Journal:  Cancers (Basel)       Date:  2019-12-13       Impact factor: 6.639

2.  Basics of particle therapy I: physics.

Authors:  Seo Hyun Park; Jin Oh Kang
Journal:  Radiat Oncol J       Date:  2011-09-30
  2 in total

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