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16F (1971AJ02)(See Energy Level Diagrams for 16F) GENERAL: See also Table 16.32 [Table of Energy Levels] (in PDF or PS). Mass of 16F: From the Q-value of the 14N(3He, n)16F reaction [Q0 = -969 ± 14 keV (1965ZA01, 1968AD03)] and the (1965MA54) masses for 14N, 3He and n, the mass excess of 16F is 10.693 ± 0.014 MeV. 16F is then unstable with respect to proton emission by 0.544 MeV. The binding energies of a deuteron, a 3He particle and an α-particle in 16F are, respectively, 10.451, 9.584 and 9.074 MeV. (1966KE16) predict M - A = 11.204 from the isobaric multiplet mass equation [the difference between this value and the experimentally observed mass excess is due to a Thomas-Ehrman shift of the unbound 16F ground state]. See also the general discussion in (1969GA1G) and (1964GA1C, 1966GA25).
Observed neutron groups are displayed in Table 16.33 (in PDF or PS) (1965ZA01, 1968AD03). Angular distributions of the neutrons corresponding to 16F*(0, 0.43, 0.72) have been measured at E(3He) = 3.5 MeV. The widths of the first four states of 16F (see Table 16.33 (in PDF or PS)) [and comparison with the analog states in 16N, 16O] suggest that Jπ for 16F*(0, 0.24, 0.43, 0.71) are (0-, 2-, 1- and 3-, respectively) [see, however, reaction 3] (1965ZA01). See also (1960BO1B, 1964BR13).
At Ep = 30 and 50 MeV, neutron groups are reported to eight excited states of 16F with Ex ≲ 19.5 MeV, including two states at Ex = 4.20 ± 0.05 and 6.16 ± 0.05 MeV (1965GR15). See also (1970WI1B).
Triton groups observed at E(3He) = 40.2 MeV are displayed in Table 16.33 (in PDF or PS). The angular distributions of the tritons to 16F*(0, 0.24) are similar, as are those of the tritons to 16F*(0.43, 0.71): comparison with analog states in 16N, 16O then suggests Jπ = 0-, 1-, 2- and 3-, respectively, for these states (1965PE04). See also (1966TO04; theor.) and (1965RI1C, 1967HA1Q).
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