Nuclear Reactions induced by the 14 MeV Neutrons
The nuclear reactions of Al, Fe, Cu, Zn, Mo and Ag produced by the neutrons from the T3(d, n) He4 reaction have been investigated by means of the activation technique. The absolute numbers of activated nuclei in samples were determined by measuring the beta-rays from the samples with a 4π-proportion...
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Published in: | Journal of the Physical Society of Japan Vol. 12; no. 5; pp. 443 - 453 |
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Main Author: | |
Format: | Journal Article |
Language: | English |
Published: |
Tokyo
The Physical Society of Japan
01-01-1957
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Online Access: | Get full text |
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Summary: | The nuclear reactions of Al, Fe, Cu, Zn, Mo and Ag produced by the neutrons from the T3(d, n) He4 reaction have been investigated by means of the activation technique. The absolute numbers of activated nuclei in samples were determined by measuring the beta-rays from the samples with a 4π-proportional counter and applying the "method of extrapolation." By utilizing the variations of neutron energies in the laboratory system, an excitation curve of Mo92(n, 2n)Mo91 reaction was obtained. For the cases of Al, Cl, Zn and Ag, only the gradients of excitation curves were also found. The experimental cross sections were determined as follows: 87.2 mb±8% for Al27(n, p)Mg27, 120 mb±12% for Al27(n, α)Na24, 144 mb±13% for Fe56(n, p)Mn56, 556 mb±5% for Cu63(n, 2n)Cu62, 119 mb±12% for Zn64(n, 2n)Zn63, 60.2 mb±12% for Zn66(n, p)Cu66, 132 mb±16% for Mo92(n, 2n)Mo91, 458mb±11% for Ag107(n, 2n)Ag106, and 604 mb±11% for Ag109(n, 2n)Ag108. Comparing these results with the predictions by the statistical theory of Weisskopf et al. it was found that they agreed with each other within about factor 3, but in details, there were some discrepancies between them. The relative behavior of excitation curve of the Mo92(n, 2n)Mo reaction seems to be consistent with the above theory, though with respect to the absolute values, the theoretical curve lies above the experimental one by about 2.4. |
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ISSN: | 0031-9015 1347-4073 |
DOI: | 10.1143/JPSJ.12.443 |