Repozytorium

The 5f2→5f16d1 absorption spectrum of Cs2GeF6:U4+ crystals: a quantum chemical and experimental study.

Autorzy

B Ordejón

Mirosław Karbowiak

Luis Seijo

Zoila Barandiarán

Rok wydania

2006

Czasopismo

Journal of Chemical Physics

Numer woluminu

125

Strony

1-9

DOI

10.1063/1.2336427

Kolekcja

Naukowa

Język

Angielski

Typ publikacji

Artykuł

Streszczenie

Single crystals of U4+-doped Cs2GeF6 with 1% U4+ concentration have been obtained by the modified Bridgman-Stockbarger method in spite of the large difference in ionic radii between Ge4+ and U4+ in octahedral coordination. Their UV absorption spectrum has been recorded at 7 K, between 190 and 350 nm; it consists of a first broad and intense band peaking at about 38 000 cm−1 followed by a number of broad bands of lower intensity from 39 000 to 45 000 cm−1. None of the bands observed shows appreciable fine vibronic structure, so that the energies of experimental electronic origins cannot be deduced and the assignment of the experimental spectrum using empirical methods based on crystal field theory cannot be attempted. Alternatively, the profile of the absorption spectrum has been obtained theoretically using the U–F bond lengths and totally symmetric vibrational frequencies of the ground 5f2−1A1g and 5f16d(t2g)1−iT1u excited states, their energy differences, and their corresponding electric dipole transition moments calculated using the relativistic ab initio model potential embedded cluster method. The calculations suggest that the observed bands are associated with the lowest five 5f2−1A1g→5f16d(t2g)1−iT1u (i = 1–5) dipole allowed electronic origins and their vibrational progressions. In particular, the first broad and intense band peaking at about 38 000 cm−1 can be safely assigned to the 0-0 and 0-1 members of the a1g progression of the 5f2−1A1g→5f16d(t2g)1−1T1u electronic origin. The electronic structure of all the states with main configurational character 5f16d(t2g)1 has been calculated as well. The results show that the lowest crystal level of this manifold is 5f16d(t2g)1−1Eu and lies about 6200 cm−1 above the 5f2 level closest in energy, which amounts to some 11 vibrational quanta. This large energy gap could result in low nonradiative decay and efficient UV emission, which suggest the interest of investigating further this new material as a potential UV solid state laser.

Adres publiczny

https://doi.org/10.1063/1.2336427

Strona internetowa wydawcy

https://www.aip.org/

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