Boron neutron capture therapy (BNCT) represents a promising modality for a
relatively selective radiation dose delivery to the tumour tissue. Boron-10
nuclei capture slow 'thermal' neutrons preferentially and, upon capture, p
romptly undergo B-10(n,alpha)Li-7 reaction. The ionization tracks of energe
tic and heavy lithium and helium ions resulting from this reaction are only
about one cell diameter in length (similar to 14 mu m). Because of their h
igh linear energy transfer (LET) these ions have a high relative biological
effectiveness (RBE) for controlling tumour growth. The key to effective BN
CT of tumours, such as glioblastoma multiforme (GBM), is the preferential a
ccumulation of boron-10 in the tumour, including the infiltrating GEM cells
, as compared with that in the vital structures of the normal brain. Provid
ed that a sufficiently high tumour boron-10 concentration (similar to 10(9)
boron-10 atoms/cell) and an adequate thermal neutron fluence (similar to 1
0(12) neutrons/ cm(2)) are achieved, it is the ratio of the boron-10 concen
tration in tumour cells to that in the normal brain cells that will largely
determine the therapeutic gain of BNCT.