Low energy neutrons (< 2 MeV), those of principal concern in radiation
protection, principally initiate recoil protons in biological tissues
. The recoil protons from monoenergetic neutrons form rectangular dist
ributions with energy. Monoenergetic neutrons of different energies (<
2 MeV) will then produce overlapping recoil proton spectra. By overla
pping the effects of individual deposition events, determined microdos
imetrically for cell nuclear dimensions, from such neutron beams the b
iological effectiveness of recoil protons within defined energy and ra
nge bounds can be determined. Here chromosomal aberrations per cell ha
ve been quantified following irradiation of Vicia faba cells with mono
energetic neutrons of 230, 320, 430, and 1,910 keV. Aberration frequen
cies from cells from part of the cell cycle, thereby limiting nuclear
dimensions, were linearly related to dose and to the frequency of prot
on recoils per nucleus. The 320 keV neutrons were the most biologicall
y effective per unit absorbed dose and 430 keV neutrons most effective
per recoil proton, with 21% of recoils inducing aberrations. After ex
traction of effectiveness per proton recoil within each energy and ran
ge bounds (0-230, 230-320, 320-430, and 430-1,910 keV), it was conclud
ed that recoil protons with energies of about 200-300 keV, traveling 2
.5-4 mu m and depositing energy at about 80 keV mu m(-1), are more eff
icient at aberration induction than those recoil protons of lesser ran
ge though near equivalent LET and those of greater range through lesse
r LET. This approach allows for assessment of the biological effective
ness of individual energy deposition events from low energy neutrons,
the lowest dose a cell can receive, and provides an alternative to con
siderations of relative biological effectiveness.