Forest He-3 Tubes

Thermal neutron capture of He-3 may be represented by the reaction below

[math]\displaystyle{ n + He^3 \rightarrow p + H^3 }[/math]

About 764 keV of energy is liberated in this nuclear reaction and distributed between the final products according to their masses. Because the proton is about a factor of 3 lighter than Tritium (H^3) , it will have more kinetic energy by about a factor of 3 (about 573 keV). This liberated proton can ionize other He-3 atoms via the reaction

[math]\displaystyle{ p+He^3 \rightarrow p + He^3(+) + e^- }[/math]

The same proton will ionize several He-3 atoms when dissipating the 573 keV kinetic energy.

The Tritium (H^3) can also ionize the gas but due to its higher mass it does not travel as far (shorter range) as the proton and makes a smaller contribution to the ionization signal.

reference: J. W. Leake, "Nuclear Instruments and Methods", Vol. 63, page 329, 1968).

The probability of neutron capture is measured in terms of a cross section. There is a nuclear data base for neutron capture located at LBL. The "free" neutron thermal cross section is about [math]\displaystyle{ 3.10 \pm 0.13 }[/math] barns ( 1 barn = [math]\displaystyle{ 10^{-24} cm^2 }[/math]).

10-atm He-3, 2.54 cm diameter tube, 76 cm long, poly moderator, cadmium metal, Boron loaded shielding.

File:He-3Tube DetectorDrawing.jpg