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16Ne (1993TI07)(See the Isobar Diagram for 16Ne)
GENERAL: See Mass of 16Ne: The Q-values of the 20Ne(α, 8He) and 16O(π+, π-) reactions lead to atomic mass excesses of 23.93 ± 0.08 MeV (1978KE06), 23.978 ± 0.024 MeV (1983WO01) and 24.048 ± 0.045 MeV (1980BU15) [recalculated using the (1985WA02) masses for 8He, 16O and 20Ne]. The weighted mean is 23.989 ± 0.020 MeV, which is also the (1985WA02) value. 16Ne is then bound with respect to decay into 15F + p by 0.07 MeV and unbound with respect to 14O + 2p by 1.40 MeV (1986AJ04).
For ground state cross sections and analyses for Eπ+ = 80 to 292 MeV see (1982AJ01, 1986AJ04). A recent measurement at θlab = 5° for Eπ+ = 140 - 292 MeV has been reported (1990SE11).
At Eα ≈ 117.5 MeV, 16Ne*(0, 1.69 ± 0.07) are populated, the former with a differential cross section of 5 ± 3 nb/sr at 8°(lab). The Γc.m. for the ground state group is 200 ± 100 keV; applying penetrability corrections leads to a total decay width of 5 - 100 keV. The di-proton branching ratio is 10 - 90%, with the most probable value being 20%. The cubic term, d, in the IMME (Isobaric Multiplet Mass Equation) is 8 ± 5 keV, 15 ± 6 keV based, respectively, on the masses of 16Ne*(0, 1.69). The first T = 2 states in 16F[0+, 2+] are predicted to lie at Ex = 10.08 ± 0.02 and 11.87 ± 0.03 MeV (1978KE06). At Eα = 129 MeV (1983WO01) find Γc.m. for 16Neg.s. = 110 ± 40 keV and the d and e coefficients in the IMME are both 4 ± 3 keV.
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