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scattering angles between 10 ◦ and 180 ◦ . Using several sets of elastic scattering phase shifts, a detailed analysis of the sharp Kr − (4p 5 5s 22 P3/2) resonance was carried out, resulting in a resonance width of Γ3/2 =3 .6(2) meV. By direct comparison with the position of the Ar − (3p 5 4s 22 P3/2) resonance, the energy for the Kr − (4p 5 5s 22 P3/2) resonance was determined as E3/2 =9 .489(3) eV. A Fano-type fit of the higher-lying Kr − (4p 5 5s 22 P1/2 )r esonance yielded the resonance parameters Γ1/2= 33(5) meV and E1/2 =1 0.126(4) eV. In order to obtain additional insight, B-spline R-matrix calculations were performed for both the elastic and the inelastic cross sections above the threshold for 4p 5 5s excitation. They provide the total and angle differential cross sections for excitation of long-lived and short lived levels of the 4p 5 5s configuration in Kr and branching ratios for the decay of the Kr − (4p 5 5s 22 P1/2) resonance into the three available exit channels. The results are compared with selected experimental data.

Electron scattering from krypton: High-resolution electron scattering experiments and B-spline R-matrix calculations