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

0436099 - ÚJF 2015 RIV NL eng J - Článek v odborném periodiku
Inoyatov, A. K. - Perevoshchikov, L. L. - Kovalík, Alojz - Filosofov, D. V. - Yushkevich, Yu. V. - Ryšavý, Miloš - Lee, B. Q. - Kibédi, T. - Stuchbery, A. E. - Zhdanov, V. S.
Influence of host matrices on krypton electron binding energies and KLL Auger transition energies.
Journal of Electron Spectroscopy and Related Phenomena. Roč. 197, DEC (2014), s. 64-71. ISSN 0368-2048. E-ISSN 1873-2526
Grant CEP: GA ČR(CZ) GAP203/12/1896; GA MŠMT LG14004
Institucionální podpora: RVO:61389005
Klíčová slova: Kr-83 * Rb-83 * Sr-83 * electron binding energy * KLL transitions * natural atomic level width * multiconfiguration Dirac-Fock calculations
Kód oboru RIV: BG - Jaderná, atomová a mol. fyzika, urychlovače
Impakt faktor: 1.436, rok: 2014

The low-energy electron spectra emitted in the radioactive decay of the Rb-83 and Sr-83 isotopes were measured with a combined electrostatic electron spectrometer. Radioactive sources used were prepared by ion implantation of 83Sr into a high purity polycrystalline platinum foil at 30 keV and by vacuum-evaporation deposition of Rb-83 on the same type of foil. From the measured conversion electron spectra, the electron binding energies for the K, L1, L2, L3, M1, M2, and M3 shell/subshells of krypton in the platinum host were determined to be 14316.4(12), 1914.3(9), 1720.3(9), 1667.6(9), 281.5(9), 209.6(13), and 201.2(15) eV, respectively, and those for the evaporated layer were observed to be lower by 0.7(1) eV. For both host matrices, values of 2.3(2), 4.6(2), 1.7(2), 1.3(2), and 3.2(3) eV were obtained for the krypton K, L1, L2, L3, and M1 natural atomic level widths, respectively. The absolute energies of 10838.5(9) and 10839.5(10) eV were measured for the KL2L3(D-1(2)) Auger transition in 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 of the KL2L3(D-1(2)) transitions in Rb and Kr in the Pt host.
Trvalý link: http://hdl.handle.net/11104/0239932