16F

Ground-State Decay Evaluated Data

Measured Ground-State Γcm for 16F

Adopted value: 40 ± 20 keV (1993TI07)
Measured Mass Excess for 16F

Adopted value: 10680 ± 8 keV (2003AU02)
Measurements
1965GR15: 16O(p, n)16F, E = 30.50 MeV; measured σ(En). 16F deduced levels.
1968AD03: 14N(3He, n), E = 3 MeV; measured Q, σ(En). 16F deduced levels.
1971ADZZ: 14N(3He, n), E = 1.73 - 3.6 MeV; measured σ(E; En, θ), Q. 16F deduced levels, mass excess.
1971MO34: 16O(p, n), E = 23 MeV; measured En. 16F deduced levels.
1971MOYY: 16O(p, n), E = 23 MeV; measured σ(En). 16F deduced levels.
1971RUZS: 16O(p, n), E = 23 MeV; measured σ(En, θ). 16F deduced levels.
1973BO50: 14N(3He, n), E = 10, 12.5, 13 MeV; measured σ(En, θ). 16F deduced levels, J, π, L.
1973BOZL: 14N(3He, n), E = 10 - 13 MeV; measured σ(θ). 16F levels deduced strength.
1974MAZZ: 14N(3He, n); measured σ(E; θ). 16F deduced levels.
1975CEZU: 16O(3He, t), E = 44 MeV; measured σ(Et, θ). 16F levels deduced J, π.
1976CEZX: 16O(3He, t), E = 44 MeV; measured σ to levels in 16F. DWBA analysis.
1976HAWZ: 14N(10B, 8Li), E = 100 MeV; measured yields. 16F deduced levels.
1976MOZD: 19F(3He, 6He), E = 35 MeV; measured σ. 16F deduced levels.
1977NA19: 16O(3He, t), E = 35 MeV; measured spectra. 16F deduced levels.
1977NAZP: 16O(3He, t), E = 35 MeV; measured σ. 16F deduced levels, J, π.
1980ANZN: 16O(p, n), E = 98.9 MeV; measured σ(θ). 16F levels deduced L, j-transfer.
1981ANZX: 16O(p, n), E = 99, 135 MeV; measured σ(En, θ). 16F deduced IAS, M1, M2, E1 transition stengths.
1981MAZW: 16O(polarized p, n), E = 135 MeV; measured σ(En, θ), A(θ). Tof. DWIA analysis.
1982AN08: 16O(p, n), E = 62 - 160 MeV; analyzed σ(θ = 0°) vs E. 16F level deduced σ/B(M1).
1982FA06: 16O(p, n), E = 99.1, 135.2 MeV; measured σ(En) vs θ; deduced σ(θ). 16F levels deduced J, π, analog character. Tof. Shell model.
1982MA11: 16O(polarized p, n), E = 134 MeV; measured σ(θ), σ(En), A(θ). 16F level deduced configuration. DWIA.
1982OH03: 16O(p, n), E = 35 MeV; measured σ(En), σ(θ); deduced giant multipole resonance virtual excitation. 16F level deduced J, π, T. DWBA, shell model.
1982OR04: 16O(p, n), E = 35 MeV; measured σ(En), σ(θ). 16F levels deduced J, π. DWBA analysis.
1982STZV: 16O(3He, t), E = 81 MeV; measured σ(Et), σ(θ). 16F levels deduced J, π, configuration. Microscopic DWBA analysis.
1982TA05: 16O(3He, t), E = 130, 170 MeV; measured σ(Et), σ(E(3He)), σ(θ). 16F deduced IAS of T = 1, GDR.
1983FAZZ: 16O(p, n), E = 99.1, 135.2 MeV; measured σ(θ). 16O(polarized p, n), E = 134 MeV; measured analyzing power vs θ. 16F levels deduced J, π. Shell model.
1983MAZG: 16O(p, n), E = 80 MeV; measured σ(En), σ(θ); deduced 0+ to 0- isovector transition. 16F deduced low-lying weakly excited level energies.
1983STZT: 16O(3He, t), E = 81 MeV; measured σ(Et), pt-coin, tp(θ). 16F deduced levels, transfer L, tentative J, π, IAS.
1984ST10: 16O(3He, t), E = 81 MeV; measured σ(Et, θt), σ(Et, θt, Ep, θp). 16F deduced levels, widths, L, J, π, decay. DWBA analysis.
1984VA43: 16O(3He, t), E = 75, 81 MeV; measured σ(Et, θt), σ(θt). 16F deduced transition strengths.
1984VAZR: 16O(3He, t), E = 75, 81 MeV; measured σ(θ), pt(θ). 16F deduced isovector ΔL = 1 strength.
1985FLZZ: 16O(p, n), E = 80 MeV; measured σ(En, θ); deduced σ(θ). 16F deduced T = 1, 0+ → 0- transition. Tof.
1985GRZV: 16O(3He, t), E = 81 MeV; measured σ(Et); deduced Q-value systematics.
1985HA01: 14N(3He, np), E = 10.5, 12 MeV; measured np-coin, σ(En, θ1, θ2). 16F deduced levels, Γ, J, L, T.
1986FLZY: 16O(p, n), E = 79.3 MeV; measured σ(θ). 16F levels deduced absolute excitation σ. DWIA analysis.
1986RYZZ: 14N(3He, n), E not given; measured np(θ). 16F levels deduced J, π.
1987AZZY: 15N(polarized p, π-), E = 200 MeV; measured σ(θ), analyzing power. 16F deduced levels, J, π.
1987JE02: 16O(γ, π-), E = 200 - 350 MeV; measured pion spectra; deduced σ(Eπ, θπ). 16F levels deduced production ratio.
1987OH04: 16O(p, n), E = 35, 40 MeV; measured σ(θ). DWBA analysis.
1987RYZZ: 14N(3He, n), E = 5, 5.45, 6.25 MeV; measured np(θ) following residue decay. 16F levels deduced Γp.
1991JA04: 16O(3He, t), E = 76.5 MeV; measured σ(Et); deduced Q-values for transitions to IAS.
1992KU24: 20Na(β+)(α); measured β-delayed particle spectra.
1992KUZO: 20Na(β+)(α); measured Eα.
1992WAZS: 16O(polarized p, n), E = 135 MeV; measured analyzing power.
1993WAZJ: 16O(polarized p, n), E = 135 MeV; measured σ(En, θ), analyzing power.
1994ME07: 16O(p, n), E = 494 MeV; measured σ(θ); deduced transition multipole components for ΔL = 0, ΔL = 1, ΔL ≥ 2. 16F deduced Gamow-Teller strength B(GT).
1994WA24: 16O(polarized p, n), E = 135 MeV; measured spin observable D(NN')(θ); analyzed σ(θ) vs excitation, 0° neutron spectra data. 16F deduced spin dipole resonance features.
1997MA68: 16O(p, n), E = 79 MeV; measured σ(θ, En), σ(θ). Comparison with DWIA calculations.
2006STZZ: 1H(15O, p), Ecm = 0.46 - 1.08 MeV; measured excitation function. 16F deduced level energies, J, π, widths.
2007LE26: 1H(15O, p), E = 120 MeV; measured excitation function. 16F deduced level widths.
2009FU03: 16O(3He, t), E = 140 MeV/nucleon; measured triton spectra, σ, angular distributions. 16F; deduced levels, J, π, widths.
2011WA17: 16O(pol. p, n)16F, E = 296 MeV; measured E(n), I(n), polarized neutrons, TOF, cross section spectrum, analyzing powers, polarized σ. Comparison with DWIA calculations. 16F; deduced levels, J, π, Gamow-Teller and spin-dipole states.
2014ST14: 1H(15O, p), E = 1.2 MeV/nucleon; measured Ep, Ip, differential σ(E). 16F; deduced levels, resonances, J, π, proton widths, S(p), spectroscopic factors.
2014WU03: 15N(7Li, 6Li), E = 34.5, 44 MeV; measured particle spectra, elastic and inelastic σ(θ). 16F; deduced proton and single-particle widths, spectroscopic factors for first four levels from mirror analogy with 16N.
2017BR07: 9Be(17Ne, 16F), E = 58 MeV/nucleon; 16F deduced levels.
2018CH25: 9Be(17Ne, 17Ne'), E = 62.9 MeV/nucleon; measured reaction products, Ep and Ip(θ). 16F; deduced invariant mass spectra, widths of the first 0-, 1-, 2-, and 3- resonances. 16F(p); deduced width of the ground state from magnitude of the final-state interactions between the protons emitted by the excited state of 17Ne.

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Last modified: 30 June 2021