Neutron resonance parameters of ⁵⁵Mn from Reich-Moore analysis of recent experimental neutron transmission and capture cross sections

High-resolution neutron capture cross section measurements of ⁵⁵Mn were recently performed at GELINA by Schillebeeckx et al. (2005) and at ORELA by Guber et al. (2007). The analysis of the experimental data was performed with the computer code SAMMY using the Bayesian approach in the resonance parameters representation of the cross sections. The neutron transmission data taken in 1988 by Harvey et al. (2007) and not analyzed before were added to the SAMMY experimental data base. More than 95% of the s-wave resonances and more than 85% of the p-wave resonances were identified in the energy range up to 125 keV, leading to the neutron strength functions S ₀ = (3.90 ± 0.78) × 10^-4 and S₁ = (0.45 ± 0.08) × 10^-4. About 25% of the d-wave resonances were identified with a possible strength function of S₂ = 1.0 × 10^-4. The capture cross section calculated at 0.0253 eV is 13.27 b, and the capture resonance integral is 13.52 ± 0.30 b. In the energy range 15 to 120 keV, the average capture cross section is 12% lower than Lerigoleur value and 25% smaller than Macklin value. GELINA and ORELA experimental capture cross sections show a background cross section not described by the Reich-Moore resonance parameters. Part of this background could be due to a direct capture component and/or to the missing d-wave resonances. The uncertainty of 10% on the average capture cross section above 20 keV is mainly due to the inaccuracy in the calculation of the background components.