E(level): From least-squares fit to Adopted Eγ data when available. In other cases weighted averages are taken of values available from different reactions

J^π(level): From the comparison of the DWBA prediction of cross section with experimental data in particle-transfer reactions or/and from angular distribution measurements of γ-rays or/and from the R-matrix analysis of the resonance data. In particle-transfer reactions, target Jπ=0⁺ for ³²S in (d,p) reaction, Jπ=0⁺ for ³⁴S in (p,d) and (d,t) reactions, Jπ=1/2- for ²⁹Si in (⁶Li,d) reaction, Jπ=3/2⁺ for ³⁵Cl in (p,³He) and (d,α) reactions. When assigning Jπ to a level based on γ transition from a level to a level of known Jπ, evaluators use the following rules: if Eγ<4 MeV, transitions are only considered to be E1,M1 or E2; if Eγ>4 MeV, M2 and E3 are considered to be possible.

T_1/2(level): From (α,nγ) and/or (d,pγ) using DSAM (Doppler shift attenuation method). Weighted averages taken when values from both are available. Level widths given are the sum of the neutron widths and gamma widths extracted from the R-Matrix analysis of the resonance data of (n,γ), unless otherwise noted.

E(γ): Values with ΔE are primarily from (α,nγ) and/or (n,γ) (E=thermal). Weighted averages taken when the quoted uncertainties are comparable in the two reactions. Others are deduced from level-energy differences.

I(γ): Primarily from (α,nγ), (d,pγ) and (n,γ). Weighted average taken when Iγ are available from more than one reference, unless otherwise noted.

M(γ): From (α,nγ) and/or (δ,pγ) by γ(θ) or γγ(θ). γ(θ) or γγ(θ) give d and Q; M1 and E2, or, E1 and M2 have been used when spin-parities are established from other methods.