6 research outputs found
Annual Catalogue of the Minnesota State Normal School at Moorhead. Seventh Year. (1894-1895)
https://red.mnstate.edu/bulletins/1064/thumbnail.jp
Modulation of the Slow Relaxation of the Magnetization Dynamics through Second Coordination Sphere in Macrocyclic Dysprosium(III) Complexes
Single-molecule
magnets (SMMs) exhibit unique magnetic properties
related to the molecular nature of these “isolated”
coordination complexes. In this study, we investigate the influence
of counterions on two macrocyclic dysprosium-based SMMs, namely, [DyLN6(OAc)2][OAc] (1) and [DyLN6(OAc)2][B(C6H5)4] (2) (LN6 = 2,7,13,18-tetramethyl-3,6,14,17,23,24-hexaazatricyclo[17.3.1.18,12]tetracosa 1(23),2,6,8,10,12(24),13,17,19,21-decaene, OAc
= acetate), differing by the nature of the counterion. We demonstrate
that the nature of the counterion indirectly modulates the degree
of coordination geometry distortion, particularly in macrocycle folding,
through subtle intermolecular interactions. This subsequently affects
the slow relaxation dynamics, as supported by both magnetic and theoretical
calculations. A noticeable decrease in the transverse magnetic anisotropy
is observed for 2, attributed to a reduced degree of
macrocycle distortion in the equatorial plane. Theoretical calculations
further suggest a greater crystal-field splitting in 2 with the first excited state estimated to be twice as large in energy
compared to 1. Both complexes exhibit magnetization relaxation
dynamics primarily driven by a Raman process
Pressure-Induced Insertion of Ammonia Borane in the Siliceous Zeolite, Silicalite-1F
A combination
of Raman spectroscopy and X-ray diffraction was used
to investigate the insertion of ammonia borane in the 5.5 Å diameter
pores of the hydrophobic, all-silica zeolite, silicalite-1F in the
pressure range up to 4.8 GPa. Insertion and nanoconfinement result
in the appearance of new Raman modes, especially in the N–H
stretching region and significant changes in the intensities and pressure
dependencies of a large number of other modes. Orientational disorder
of the −BH<sub>3</sub> and −NH<sub>3</sub> groups persists
to higher pressures in nanoconfined as compared to the bulk ammonia
borane. The structure of the recovered sample was determined by single
crystal X-ray diffraction. Each pore in the unit cell was found to
contain between 2 and 3 molecules of ammonia borane forming single-molecule
chains due to the spatial constraints. In situ, high pressure, X-ray
powder diffraction indicated that the compressibility of the ammonia
borane-silicalite-1F composite is three times lower than that of empty
silicalite-1F due to pore filling. These results show that silicalite-1F
can be a suitable nanoscaffold for this important chemical hydrogen-storage
material
Mechanism of H<sub>2</sub>O Insertion and Chemical Bond Formation in AlPO<sub>4</sub>‑54·<i>x</i>H<sub>2</sub>O at High Pressure
The
insertion of H<sub>2</sub>O in AlPO<sub>4</sub>-54·<i>x</i>H<sub>2</sub>O at high pressure was investigated by single-crystal
X-ray diffraction and Monte Carlo molecular simulation. H<sub>2</sub>O molecules are concentrated, in particular, near the pore walls.
Upon insertion, the additional water is highly disordered. Insertion
of H<sub>2</sub>O (superhydration) is found to impede pore collapse
in the material, thereby strongly modifying its mechanical behavior.
However, instead of stabilizing the structure with respect to amorphization,
the results provide evidence for the early stages of chemical bond
formation between H<sub>2</sub>O molecules and tetrahedrally coordinated
aluminum, which is at the origin of the amorphization/reaction process
Saturation of the Siliceous Zeolite TON with Neon at High Pressure
The
insertion of neon and argon in the 1-D pore system of the zeolite
TON was studied at high pressure by X-ray diffraction and by Monte
Carlo (MC) molecular modeling. Rietveld refinements of the crystal
structure of TON and the MC results indicate that 12 Ne atoms enter
the unit cell of TON, completely filling the pores. This is much greater
than the degree of filling observed for argon, which due to size considerations
lies in a vertical plane in the pores. A phase transition from the <i>Cmc</i>2<sub>1</sub> to a <i>Pbn</i>2<sub>1</sub> structure
occurs at 0.6 GPa with cell doubling. The compressibility and structural
distortions, such as pore ellipticity, are considerably reduced as
compared to the argon-filled or the empty-pore material. In addition,
the crystalline form persists to pressures of the order of 20 GPa,
and the <i>Pbn</i>2<sub>1</sub> phase is recovered after
decompression. The results show the very strong and different effects
of pore filling by noble gases on the structural stability and mechanical
properties of this prototypical 1-D zeolite-type material
High-Pressure Phase Transition, Pore Collapse, and Amorphization in the Siliceous 1D Zeolite, TON
The siliceous zeolite
TON with a 1-D pore system was studied at
high pressure by X-ray diffraction, infrared spectroscopy, and DFT
calculations. The behavior of this material was investigated using
nonpenetrating pressure-transmitting media. Under these conditions,
a phase transition from the <i>Cmc</i>2<sub>1</sub> to a <i>Pbn</i>2<sub>1</sub> structure occurs at close to 0.6 GPa with
doubling of the primitive unit cell based on Rietveld refinements.
The pores begin to collapse with a strong increase in their ellipticity.
Upon decreasing the pressure below this value the initial structure
was not recovered. DFT calculations indicate that the initial empty
pore <i>Cmc</i>2<sub>1</sub> phase is dynamically unstable.
Irreversible, progressive pressure-induced amorphization occurs upon
further increases in pressure up to 21 GPa. These changes are confirmed
in the mid- and far-infrared spectra by peak splitting at the <i>Cmc</i>2<sub>1</sub> to <i>Pbn</i>2<sub>1</sub> phase
transition and strong peak broadening at high pressure due to amorphization