Abstract

From recent experiments it seems very probable that the 6.2-Mev quanta from the proton bombardment of fluorine are associated in one-to-one correspondence with the short range alpha-particles. This correspondence makes possible the establishment of the gamma-ray intensity by measuring the alpha-particle yield. With a specially designed variable pressure absorption-cell ionization-chamber to facilitate clear distinction between the short range alpha-particles and the scattered protons, the angular distribution and total yield of the alpha-particles at the lowest resonance (330 kv) have been determined. The determinations were based on plateaus appearing in curves of counting rate as a function of (1) cell pressure, (2) counter bias, and (3) bombarding voltage at angles of 60\ifmmode^\circ\else\textdegree\fi{}, 90\ifmmode^\circ\else\textdegree\fi{}, 120\ifmmode^\circ\else\textdegree\fi{}, and 150\ifmmode^\circ\else\textdegree\fi{} with respect to the proton beam. The results show that: ($a$) To within two percent the angular distribution of the alpha-particles is spherically symmetric; and ($b$) the yield over $4\ensuremath{\pi}$ steradians is 8.9\ifmmode\pm\else\textpm\fi{}0.5\ifmmode\times\else\texttimes\fi{}${10}^{4}$ alpha-particles per microcoulomb of 360-kv protons bombarding a thick crystal of Ca${\mathrm{F}}_{2}$. The absolute number of quanta from the reaction is presumably the same to the same accuracy. With both a heavily shielded counter and a similarly protected electroscope the ratio of the gamma-ray intensity at 1050 kv to that at 370 kv was found to be 42.0\ifmmode\pm\else\textpm\fi{}0.8. Thus the gamma-ray intensity at 1050-kv bombarding voltage is ${3.7}_{4}$\ifmmode\pm\else\textpm\fi{}0.2\ifmmode\times\else\texttimes\fi{}${10}^{6}$ quanta per microcoulomb of protons on Ca${\mathrm{F}}_{2}$. The angular distribution of the gamma-radiation was found to be spherically symmetric to within the experimental error of five percent. Knowledge of the absolute intensity of the fluorine source greatly enhances its value in photo-nuclear and other experiments.

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