Einsteinium atomic properties

Edison storage battery, 406 Einstein, Albert, 121 Einsteinium, oxidation number, 414 Elastic collision, 6 Electrical nature of atoms, 236 Electrical phenomena, 74 Electrical properties of condensed phases, 78... 

Mendelevium — (Dmitri Mendeleev [1834-1907]), Md at. wt. (258) at. no. 101 m.p. 827°C valence +2, +3. Mendelevium, the ninth transuranium element of the actinide series to be discovered, was first identified by Ghiorso, Harvey, Choppin, Thompson, and Seaborg early in 1955 as a result of the bombardment of the isotope Es with helium ions in the Berkeley 60-inch cyclotron. The isotope produced was Md, which has a half-life of 78 min. This first identification was notable in that Md was synthesized on a one-atom-at-a-time basis. Nineteen isotopes and isomers are now recognized. Md has a half-life of 51.5 days. This isotope has been produced by the bombardment of an isotope of einsteinium with ions of helium. It now appears possible that eventually enough Md can be made so that some of its physical properties can be determined. Md has been used to elucidate some of the chemical properties of mendelevium in aqueous solution. Experiments seem to show that the element possesses a moderately stable dipositive (II) oxidation state in addition to the tripositive (III) oxidation state, which is characteristic of actinide elements. 

Fujita, D. K. (1969) Some Magnetic, Spectroscopic, and Crystallographic Properties of Berkelium, Californium and Einsteinium (PhD Thesis), US Atomic Energy Commission Document UCRL-19507, University of California, Lawrence Berkeley Radiation Laboratory. 

The primary nuclear properties of the known isotopes of einsteinium are listed in Table 12.1 (see also refs 2 and 3). From detailed studies of their nuclear decay, the nuclear levels of their daughters have been obtained and the precise atomic mass... 

Photoionization detection in a buffer gas has also been used to study the properties of superheavy (transuranium) elements with charge numbers Z > 92. Isotopes of such elements can only be produced by fission reactions in heavy-ion collisions or by transfer reactions using radioactive targets. The elements produced can be placed in an optical buffer-gas cell for the purpose of laser resonance photoionization spectroscopy. This was successfully demonstrated with atoms of such radioactive elements as americium (Z = 95) (Backe et al. 2000), einsteinium (Z = 99) (Kohler et al. 1997), and fermium (Z = 100) (Sewtz et al. 2003). 

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