1994
DOI: 10.1016/0360-3016(94)90486-3
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Methods for radiation dose distribution analysis and treatment planning in boron neutron capture therapy

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Cited by 48 publications
(33 citation statements)
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“…Epithermal beams, with energies 0.5 eV to 10 keV, have better penetration in tissues. 1) Although the probability of reaction of an epithermal neutron with 10 B is much smaller than that of a thermal neutron, as they lose energy with tissue depth, they fall into the thermal range which is so much more effective in the boron neutron capture reaction. The peak of this thermalization of epithermal neutrons is about 3 cm in depth.…”
mentioning
confidence: 99%
“…Epithermal beams, with energies 0.5 eV to 10 keV, have better penetration in tissues. 1) Although the probability of reaction of an epithermal neutron with 10 B is much smaller than that of a thermal neutron, as they lose energy with tissue depth, they fall into the thermal range which is so much more effective in the boron neutron capture reaction. The peak of this thermalization of epithermal neutrons is about 3 cm in depth.…”
mentioning
confidence: 99%
“…The low neutron yield of the DD reaction is an obstacle for its use in this particular therapy. Neutrons from the Neutron source 3 H(d n) 4 He 2 H(d n) 3 He 7 Li(p n) 7 Be 7 Li(p n) 7 DT reaction could be moderated to around 10 keV without reducing the neutron ux to a negligible level. An equivalent tumor dose of 21.9 Gy-Eq could be achieved at a depth of 8 cm in the head pantom, which is about 50% higher than doses obtained by a neutron beam currently used at BMRR for clinical trials.…”
Section: Discussionmentioning
confidence: 99%
“…The optimal combination of materials that we came up with for DD was 30 cm of 7 LiF and 18 cm of 40%Al/60%AlF 3 . The BSA is 25 cm in diameter and surrounded by a thin (0.5 mm) layer of 6 …”
Section: Optimal Bsa and Dose Distribution For Ddmentioning
confidence: 99%
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“…Analyzing the transport of neutrons and photons through a head phantom is necessary to determine the clinical properties of a beam. This has been done in the second modeling stage using the Monte Carlo-based BNCT treatment planning code, "rtt-MC" [2]. The geometry and setup is depicted in figure 1.…”
Section: Moderator and Neutron Transport Modelingmentioning
confidence: 99%