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