The absolute yield, angular distribution and resonance widths of the 6.13, 6.92 and 7.12 MeV photons from the 340.5 keV resonance of the 19F(p,αγ)16O reaction
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Cited by (27)
α-particle induced yield of 6.13 MeV γ-rays in carbon
2021, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentComments on extracting the resonance strength parameter from yield data
2015, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentThe yields, branching ratios and angular distributions of 6-7 MeV photons produced in the <sup>19</sup>F(p,αγ)<sup>16</sup>O reaction
2002, Applied Radiation and IsotopesThick target photon yields and angular distributions for the <sup>19</sup>F(p,αγ)<sup>16</sup>O source reaction at incident proton energies between 1.5 and 4.0 MeV
2000, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentObservation of uranium photo-fission by <sup>16</sup>N decay gamma rays from water activated by D-T fusion neutrons
2000, Fusion Engineering and DesignCitation Excerpt :In both instances the gamma rays follow the prompt radiative decay of excited levels in 16O. Some physical features of the 19F(p, α–γ)16O reaction, such as individual resonance parameters and both thick and thin target gamma-ray yields as a function of incident proton energy, have been studied and reported in the literature ([11–14]). This process has been exploited in developing a micro-analysis technique for the quantitative determination and depth profiling of fluorine in the surface region of various substrates (e.g. Refs. [12] and [14]).
A compilation of charged-particle induced thermonuclear reaction rates
1999, Nuclear Physics A
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