2 research outputs found

    Electronic Structure of the Complete Series of Gas-Phase Manganese Acetylacetonates by X‑ray Absorption Spectroscopy

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    Metal centers in transition metal–ligand complexes occur in a variety of oxidation states causing their redox activity and therefore making them relevant for applications in physics and chemistry. The electronic state of these complexes can be studied by X-ray absorption spectroscopy, which is, however, due to the complex spectral signature not always straightforward. Here, we study the electronic structure of gas-phase cationic manganese acetylacetonate complexes Mn(acac)1–3+ using X-ray absorption spectroscopy at the metal center and ligand constituents. The spectra are well reproduced by multiconfigurational wave function theory, time-dependent density functional theory as well as parameterized crystal field and charge transfer multiplet simulations. This enables us to get detailed insights into the electronic structure of ground-state Mn(acac)1–3+ and extract empirical parameters such as crystal field strength and exchange coupling from X-ray excitation at both the metal and ligand sites. By comparison to X-ray absorption spectra of neutral, solvated Mn(acac)2,3 complexes, we also show that the effect of coordination on the L3 excitation energy, routinely used to identify oxidation states, can contribute about 40–50% to the observed shift, which for the current study is 1.9 eV per oxidation state

    Size-Dependent Ligand Quenching of Ferromagnetism in Co<sub>3</sub>(benzene)<sub><i>n</i></sub> <sup>+</sup> Clusters Studied with X‑ray Magnetic Circular Dichroism Spectroscopy

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    Cobalt–benzene cluster ions of the form Co<sub>3</sub>(bz)<sub><i>n</i></sub> <sup>+</sup> (<i>n</i> = 0–3) were produced in the gas phase, mass-selected, and cooled in a cryogenic ion trap held at 3–4 K. To explore ligand effects on cluster magnetic moments, these species were investigated with X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD) spectroscopy. XMCD spectra yield both the spin and orbital angular momenta of these clusters. Co<sub>3</sub> <sup>+</sup> has a spin magnetic moment of μ<sub>S</sub> = 6 μ<sub>B</sub> and an orbital magnetic moment of μ<sub>L</sub> = 3 μ<sub>B</sub>. Co<sub>3</sub>(bz)<sup>+</sup> and Co<sub>3</sub>(bz)<sub>2</sub> <sup>+</sup> complexes were found to have spin and orbital magnetic moments identical to the values for ligand-free Co<sub>3</sub> <sup>+</sup>. However, coordination of the third benzene to form Co<sub>3</sub>(bz)<sub>3</sub> <sup>+</sup> completely quenches the high spin state of the system. Density functional theory calculations elucidate the spin states of the Co<sub>3</sub>(bz)<sub><i>n</i></sub> <sup>+</sup> species as a function of the number of attached benzene ligands, explaining the transition from septet to singlet for <i>n</i> = 0 → 3
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