Energy spectra and absolute differential cross sections of protons from bombardment of ${\mathrm{F}}^{19}$ with 21.4- and 27.4-Mev ${\mathrm{N}}^{14}$ were measured. The energy spectra were analyzed in terms of the statistical model with a level density $\mathrm{exp}(\frac{{E}^{*}}{T})$, where ${E}^{*}$ is the excitation energy in the residual nucleus of the assumed reaction ${\mathrm{F}}^{19}({\mathrm{N}}^{14}, p){P}^{32}$. The nuclear temperature $T$ increased from about 1.9 Mev at 0\ifmmode^\circ\else\textdegree\fi{} to about 2.5 Mev at 145\ifmmode^\circ\else\textdegree\fi{} c.m., but did not vary with bombarding energy. The angular distribution show minima near 90\ifmmode^\circ\else\textdegree\fi{} c.m., with anisotropy increasing as the bombarding energy and proton energy increase. At the lower bombarding energy there is approximate agreement with the Ericson-Strutinski theory of angular-momentum effects in compound-nucleus processes, over the entire observed ranges of angle and proton energy. The fit is consistent with $\ensuremath{\sigma}=3$ in the nuclear level spin distribution $(2j+1)\mathrm{exp}[\ensuremath{-}\frac{j(j+1)}{(2{\ensuremath{\sigma}}^{2})}]$. At the higher bombarding energy a considerable excess of protons are emitted into the backward hemisphere, especially at high proton energies, suggesting a direct-interaction mechanism in which the observed proton comes from the ${\mathrm{F}}^{19}$.
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