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Geometric, electronic and magnetic structure of Fe$_{x}$O$_{y}^{+}$ clusters

Published 8 Jun 2015 in physics.atm-clus | (1506.02532v2)

Abstract: Correlation between geometry, electronic structure and magnetism of solids is both intriguing and elusive. This is particularly strongly manifested in small clusters, where a vast number of unusual structures appear. Here, we employ density functional theory in combination with a genetic search algorithm, GGA$+U$ and a hybrid functional to determine the structure of gas phase Fe${x}$O${y}{+/0}$ clusters. For Fe${x}$O${y}$ cation clusters we also calculate the corresponding vibration spectra and compare them with experiments. We successfully identify Fe${3}$O${4}{+}$, Fe${4}$O${5}{+}$, Fe${4}$O${6}{+}$, Fe${5}$O${7}{+}$ and propose structures for Fe${6}$O${8}{+}$. Within the triangular geometric structure of Fe${3}$O${4}{+}$ a non-collinear, ferrimagnetic and ferromagnetic state are comparable in energy. Fe${4}$O${5}{+}$ and Fe${4}$O${6}{+}$ are ferrimagnetic with a residual magnetic moment of 1~\muB{} due to ionization. Fe${5}$O${7}{+}$ is ferrimagnetic due to the odd number of Fe atoms. We compare the electronic structure with bulk magnetite and find Fe${4}$O${5}{+}$, Fe${4}$O${6}{+}$, Fe${6}$O${8}{+}$ to be mixed valence clusters. In contrast, in Fe${3}$O${4}{+}$ and Fe${5}$O${7}{+}$ all Fe are found to be trivalent.

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