Difference between revisions of "Forest He-3 Tubes"
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| − | The probability of neutron capture is measured in terms of a cross section. There is a nuclear data base for neutron capture located at [http://ie.lbl.gov/ng.html LBL] | + | The probability of neutron capture is measured in terms of a cross section. There is a nuclear data base for neutron capture located at [http://ie.lbl.gov/ng.html LBL]. The "free" neutron thermal cross section is about [http://ie.lbl.gov/ngdata/sig.htm <math>3.10 \pm 0.13</math>] barns ( 1 barn = <math>10^{-28} cm^2</math>). |
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[[Image:He-3Tube_DetectorDrawing.jpg]] | [[Image:He-3Tube_DetectorDrawing.jpg]] | ||
[[Image:He-3Tube_PPND_Efficiency.jpg | 200 px]] | [[Image:He-3Tube_PPND_Efficiency.jpg | 200 px]] | ||
Revision as of 10:03, 6 June 2008
Thermal neutron capture of He-3 may be represented by the reaction below
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
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 barns ( 1 barn = ).
File:He-3Tube DetectorDrawing.jpg
