5 research outputs found
Optical Spectra and Magnetic Behavior of a Wide Range of Europium(III) Oxo-Compounds: Analysis of the Ligand-Field Effects
The
europiumâoxygen interaction in nine different europiumÂ(III)
oxo-compounds (including <i>C</i>-type Eu<sub>2</sub>O<sub>3</sub>) was investigated on the basis of powder reflectance spectra
(near-IR/vis/UV) and temperature-dependent magnetic measurements.
Computation of the transition energies and of the effective Bohr magneton
numbers for Eu<sup>3+</sup> in the different ligand fields were performed
within the framework of the <i>angular overlap model</i> (AOM) using the computer program BonnMag. These calculations show
that all electronic transition energies in the optical spectra, the
magnetic susceptibilities as well as their temperature dependence,
are very well-accounted for by AOM. BonnMag provides a facile way
to perform these calculations. Analysis of the obtained âbest
fitâ AOM parameters <i>e</i><sub>Ď</sub>(Eu<sup>III</sup>âO) shows that these are significantly influenced
by the further bonding partners of oxygen (âsecond-sphere ligand-field
effectâ). An increase of <i>e</i><sub>Ď, max</sub>(Eu<sup>III</sup>âO) from 404 cm<sup>â1</sup> (EuPO<sub>4</sub>) to 687 cm<sup>â1</sup> (EuSbO<sub>4</sub>), both
normalized to <i>d</i>(Eu<sup>III</sup>âO) = 2.38
Ă
, is found. Correlation of this variation to oxide polarizability
and optical basicity of the oxo-compounds is discussed
The Electronic States of U<sup>4+</sup> in U(PO<sub>4</sub>)Cl: An Example for Angular Overlap Modeling of 5f<sup><i>n</i></sup> Systems
Detailed
experimental data on UPO<sub>4</sub>Cl comprising single-crystal UV/vis/NIR
spectra and temperature-dependent magnetic susceptibilities form the
basis for the investigation of the electronic structure of the U<sup>4+</sup> cation in UPO<sub>4</sub>Cl. For modeling of the observed
physical properties the <i>angular overlap model</i> (AOM)
was successfully employed. The computations were performed using the
newly developed computer program BonnMag. The calculations show that
all electronic transitions and the magnetic susceptibility as well
as its temperature dependence are well-reproduced within the AOM framework.
Using JuddâOfelt theory BonnMag allows estimation of the relative
absorption coefficients of the electronic transitions with reasonable
accuracy. Ligand field splitting for states originating from f-electron
configurations are determined. SlaterâCondonâShortley
parameters and the spinâorbit coupling constant for U<sup>4+</sup> were taken from literature. The good transferability of AOM parameters
for U<sup>4+</sup> is confirmed by calculations of the absorption
spectra of UP<sub>2</sub>O<sub>7</sub> and (U<sub>2</sub>O)Â(PO<sub>4</sub>)<sub>2</sub>. The effect of variation of the fit parameters
is investigated. AOM parameters for U<sup>4+</sup> (5f) are compared
to those of the rare-earth elements (4f) and transition metals (3d)
(Bis(terpyridine))copper(II) Tetraphenylborate: A Complex Example for the JahnâTeller Effect
The
surprisingly complicated crystal structure of (bisÂ(terpyridine))ÂcopperÂ(II)
tetraphenylborate [CuÂ(tpy)<sub>2</sub>]Â(BPh<sub>4</sub>)<sub>2</sub> (tpy = 2,2â˛:6â˛,2âł-terpyridine) consists of
six crystallographically independent [CuÂ(tpy)<sub>2</sub>]<sup>2+</sup> complexes. At ambient temperature, five out of six [Cu<sup>II</sup>N<sub>6</sub>] chromophores appear to be compressed octahedra, while
at 100 K, four exhibit elongated and only two compressed octahedral
geometry. Temperature dependent single crystal UV/vis (100, 298 K)
and EPR measurements (20, 100, 298 K) as well as AOM calculations
suggest that the octahedra which show apparently compressed octahedral
geometry (XRD) result from dynamic JahnâTeller behavior of
elongated octahedra [Cu<sup>II</sup>N<sub>6</sub>]. The detailed correlation
of structural and spectroscopic data allows an understanding of the
strongly solvent-dependent structures of the [CuÂ(tpy)<sub>2</sub>]<sup>2+</sup> complex in solution
Comprehensive Characterization of the Electronic Structure of U<sup>4+</sup> in Uranium(IV) Phosphate Chloride
Emerald-green single
crystals of UÂ(PO<sub>4</sub>)Cl were grown
by chemical vapor transport in a temperature gradient (1000 â
900 °C). The crystal structure of UÂ(PO<sub>4</sub>)Cl (<i>Cmcm</i>, <i>Z</i> = 4, <i>a</i> = 5.2289(7)
Ă
, <i>b</i> = 11.709(2) Ă
, <i>c</i> =
6.9991(8) Ă
) consists of a three-dimensional network of [PO<sub>4</sub>] tetrahedra and bicapped octahedral [U<sup>IV</sup>O<sub>6</sub>Cl<sub>2</sub>] groups. Polarized absorption spectra measured
for two perpendicular polarization directions show a large number
of well-resolved electronic transitions. These transitions can be
fully assigned on the basis of a detailed ligand-field treatment within
the framework of the <i>angular overlap model</i>. The magnetic
behavior predicted on the
basis of the spectroscopic data is in agreement with an fâŻ<sup>2</sup> system and perfectly matched by the results of temperature-dependent
susceptibility measurements
Statistical Analysis of Coordination Environments in Oxides
Coordination
or local environments (e.g., tetrahedra and octahedra)
are powerful descriptors of the crystalline structure of materials.
These structural descriptors are essential to the understanding of
crystal chemistry and the design of new materials. However, extensive
statistics on the occurrence of local environment are not available
even on common chemistries such as oxides. Here, we present the first
large-scale statistical analysis of the coordination environments
of cations in oxides using a large set of experimentally observed
compounds (about 8000). Using a newly developed method, we provide
the distribution of local environment for each cation in oxides. We
discuss our results highlighting previously known trends and unexpected
coordination environments, as well as compounds presenting very rare
coordinations. Our work complements the know-how of the solid state
chemist with a statistically sound analysis and paves the way for
further data mining efforts linking, for instance, coordination environments
to materials properties