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The low-energy electron spectra emitted in the radioactive decay of the$^{83}$Rb and $^{83}$Sr isotopes were measured with a combined electrostaticelectron spectrometer. Radioactive sources used were prepared by ionimplantation of $^{83}$Sr into a high purity polycrystalline platinum foil at30 keV and by vacuum-evaporation deposition of  $^{83}$ Rb on the same type of foil. From the measured conversion electronspectra, the electron binding energies (referenced to the Fermi level) for theK, L$_1$ , L$_2$ , L$_3$ , M$_1$ , M$_2$, and M$_3$ shell/subshells of kryptonin the platinum host were determined to be 14 316.4(12), 1 914.3(9), 1720.3(9), 1 667.6(9), 281.5(9), 209.6(13), and 201.2(15) eV, respectively, andthose for the evaporated layer were observed to be lower by 0.7(1) eV. For bothhost matrices, values of 2.3(2), 4.6(2), 1.7(2), 1.3(2), and 3.2(3) eV wereobtained for the krypton K, L$_1$ , L$_2$ , L$_3$ , and M$_1$ natural atomiclevel widths, respectively. The absolute energies of 10 838.5(9) and 10839.5(10) eV were measured for the KL$_2$L$_3$ ($^{1}$D$_2$) Auger transitionin krypton implanted in Pt and generated in the evaporated rubidium layer,respectively. A value of 601.0(8) eV was measured for the energy difference ofthe KL$_2$L$_3$ ($^{1}$D$_2$) transitions in Rb and Kr in the Pt host.Multiconfiguration Dirac-Fock calculations of the krypton KLL transitionenergies and intensities were also performed.

Influence of host matrices on krypton electron binding energies and KLL Auger transition energies