6 research outputs found
Computationally Assisted (Solid-State Density Functional Theory) Structural (X-ray) and Vibrational Spectroscopy (FT-IR, FT-RS, TDs-THz) Characterization of the Cardiovascular Drug Lacidipine
The
structural properties of a second-generation dihydropyridine calcium
antagonist, lacidipine, were explored by combining low-temperature
X-ray diffraction with optical vibrational spectroscopy and periodic
density functional theory (PBC DFT) calculations. Crystallographic
analysis cannot discriminate between two possible molecular symmetries
in crystals made of pure lacipidine: the space group <i>Ama</i>2, where the lacipidine molecule lies on mirror symmetry, or a <i>Cc</i> space group with distorted lacipidine molecules. Intermolecular
interactions analysis reveals an infinite net of moderate-strength
N–H···O hydrogen-bonds, which link the molecular
units toward the crystallographic <i>b</i>-axis. Weak interactions
were identified, revealing their role in stabilization of the crystal
structure. The vibrational dynamics of lacidipine was thoroughly explored
by combining infrared and Raman spectroscopy in the middle- and low-wavenumber
range. The given interpretation was fully supported by state-of-the-art
solid-state density functional theory calculations (plane-wave DFT),
giving deep insight into the vibrational response and providing a
complex assignment of spectral features. The vibrational analysis
was extended onto the lattice-phonon range by employing time-domain
terahertz spectroscopy. Analysis of the anisotropic displacement parameters
suggests noticeable dynamics of the terminal (<i>tert</i>-butoxycarbonyl)vinyl moiety. The terahertz study provides
direct experimental evidence of “crankshaft” type motions
in the terminal chain. By combining low-wavenumber vibrational spectroscopy
with the first-principles calculations, we were able to prove that
the quoted thermodynamically stable phase corresponds to the monoclinic <i>Cc</i> space group
Synthesis and Characterization of Redox-Active Mononuclear Fe(κ<sup>2</sup>‑dppe)(η<sup>5</sup>‑C<sub>5</sub>Me<sub>5</sub>)‑Terminated π‑Conjugated Wires
Several new redox-active Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>) arylacetylide
complexes featuring
pendant ethynyl (Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)[{CC(1,4-C<sub>6</sub>H<sub>4</sub>)}<sub><i>n</i></sub>CCH] (<b>1b</b>–<b>d</b>; <i>n</i> = 1–3), Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)[CC(1,3-C<sub>6</sub>H<sub>4</sub>)CCH] (<b>2</b>)) or ethenyl (Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)[CC(1,4-C<sub>6</sub>H<sub>4</sub>)CHCH<sub>2</sub>] (<b>3</b>))
groups have been synthesized and characterized under their Fe(II)
and Fe(III) states. In contrast to the known ethynyl Fe(III) complex
[Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(CCH)][PF<sub>6</sub>] (<b>1a</b>[PF<sub>6</sub>]), most of the new Fe(III) derivatives turned out to be kinetically
stable in solution. A consistent picture of the electronic structure
of the latter complexes in both redox states emerged from experimental
data and DFT calculations. This study revealed that beyond the first
1,4-phenylene ring, modification or extension of the carbon-rich linker
using (4-phenylene)ethynylene spacers will have only a minor influence
on their electronic properties in their ground state, while still
maintaining some
(weak) electronic interaction along the carbon-rich backbone
Synthesis and Characterization of Redox-Active Mononuclear Fe(κ<sup>2</sup>‑dppe)(η<sup>5</sup>‑C<sub>5</sub>Me<sub>5</sub>)‑Terminated π‑Conjugated Wires
Several new redox-active Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>) arylacetylide
complexes featuring
pendant ethynyl (Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)[{CC(1,4-C<sub>6</sub>H<sub>4</sub>)}<sub><i>n</i></sub>CCH] (<b>1b</b>–<b>d</b>; <i>n</i> = 1–3), Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)[CC(1,3-C<sub>6</sub>H<sub>4</sub>)CCH] (<b>2</b>)) or ethenyl (Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)[CC(1,4-C<sub>6</sub>H<sub>4</sub>)CHCH<sub>2</sub>] (<b>3</b>))
groups have been synthesized and characterized under their Fe(II)
and Fe(III) states. In contrast to the known ethynyl Fe(III) complex
[Fe(κ<sup>2</sup>-dppe)(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(CCH)][PF<sub>6</sub>] (<b>1a</b>[PF<sub>6</sub>]), most of the new Fe(III) derivatives turned out to be kinetically
stable in solution. A consistent picture of the electronic structure
of the latter complexes in both redox states emerged from experimental
data and DFT calculations. This study revealed that beyond the first
1,4-phenylene ring, modification or extension of the carbon-rich linker
using (4-phenylene)ethynylene spacers will have only a minor influence
on their electronic properties in their ground state, while still
maintaining some
(weak) electronic interaction along the carbon-rich backbone
Correlation between Metal–Insulator Transition and Hydrogen-Bonding Network in the Organic Metal δ‑(BEDT-TTF)<sub>4</sub>[2,6-Anthracene-bis(sulfonate)]·(H<sub>2</sub>O)<sub>4</sub>
The sensitivity of electronic properties
of organic conductors
to minute modifications of their solid-state structure is investigated
here within BEDT-TTF (ET) salts with organic bis-sulfonate anions,
where specific hydrogen bonds between water molecules and sulfonate
moieties are shown to dynamically control the organic slabs’
electronic structure. While the mixed-valence, 2,6-naphthalene-bis(sulfonate)
salt, (ET)<sub>4</sub>(NBS)·4H<sub>2</sub>O, exhibits
a charge order state already at room temperature, the corresponding
salt with the 2,6-anthracene-bis(sulfonate) dianion, formulated as
(ET)<sub>4</sub>(ABS)·4H<sub>2</sub>O, is metallic
at RT and exhibits a metal–insulator transition at <i>T</i><sub>MI</sub> = 85 K. The origin of the MI transition is
revealed from a combination of temperature-dependent spectroscopic
(Raman) measurements, X-ray structure elucidations (from 300 to 15
K), and theoretical investigations, demonstrating that the charge
disproportionation observed below <i>T</i><sub>MI</sub> is
associated here with the progressive switching of bifurcated OH···O
hydrogen bonds between the sulfonate moieties of the anion and the
trapped water molecules. These movements within the anion layer are
transmitted through weaker C–H···O interactions
to the two A and B donor molecules, modifying the details of the overlap
interactions within AA and BB pairs and opening a gap in the band
structure
Correlation between Metal–Insulator Transition and Hydrogen-Bonding Network in the Organic Metal δ‑(BEDT-TTF)<sub>4</sub>[2,6-Anthracene-bis(sulfonate)]·(H<sub>2</sub>O)<sub>4</sub>
The sensitivity of electronic properties
of organic conductors
to minute modifications of their solid-state structure is investigated
here within BEDT-TTF (ET) salts with organic bis-sulfonate anions,
where specific hydrogen bonds between water molecules and sulfonate
moieties are shown to dynamically control the organic slabs’
electronic structure. While the mixed-valence, 2,6-naphthalene-bis(sulfonate)
salt, (ET)<sub>4</sub>(NBS)·4H<sub>2</sub>O, exhibits
a charge order state already at room temperature, the corresponding
salt with the 2,6-anthracene-bis(sulfonate) dianion, formulated as
(ET)<sub>4</sub>(ABS)·4H<sub>2</sub>O, is metallic
at RT and exhibits a metal–insulator transition at <i>T</i><sub>MI</sub> = 85 K. The origin of the MI transition is
revealed from a combination of temperature-dependent spectroscopic
(Raman) measurements, X-ray structure elucidations (from 300 to 15
K), and theoretical investigations, demonstrating that the charge
disproportionation observed below <i>T</i><sub>MI</sub> is
associated here with the progressive switching of bifurcated OH···O
hydrogen bonds between the sulfonate moieties of the anion and the
trapped water molecules. These movements within the anion layer are
transmitted through weaker C–H···O interactions
to the two A and B donor molecules, modifying the details of the overlap
interactions within AA and BB pairs and opening a gap in the band
structure
2,7-Fluorenediyl-Bridged Complexes Containing Electroactive “Fe(η<sup>5</sup>‑C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>‑dppe)CC–” End Groups: Molecular Wires and Remarkable Nonlinear Electrochromes
The 2,7-fluorenyl-bridged Fe(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>-dppe)[CC(2,7-C<sub>13</sub>H<sub>6</sub>Bu<sub>2</sub>)CC]Fe(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>-dppe) (<b>1a</b>), its
extended analogue Fe(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>-dppe)[CC(1,4-C<sub>6</sub>H<sub>4</sub>)CC(2,7-C<sub>13</sub>H<sub>6</sub>Bu<sub>2</sub>)CC(1,4-C<sub>6</sub>H<sub>4</sub>)CC](η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>-dppe)Fe (<b>1b</b>), and
the corresponding mononuclear complexes Fe(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>-dppe)[CC(2-C<sub>13</sub>H<sub>7</sub>Bu<sub>2</sub>)] (<b>2a</b>) and Fe(η<sup>5</sup>-C<sub>5</sub>Me<sub>5</sub>)(κ<sup>2</sup>-dppe)[CC(1,4-C<sub>6</sub>H<sub>4</sub>)CC(2-C<sub>13</sub>H<sub>7</sub>Bu<sub>2</sub>)] (<b>2b</b>), which model half of these molecules,
have been synthesized and characterized in their various redox states.
The molecular wire characteristics of the dinuclear complexes were
examined in their mixed-valent states, with progression from <b>1a</b>[PF<sub>6</sub>] to <b>1b</b>[PF<sub>6</sub>] resulting
in a sharp decrease in electronic coupling. The cubic nonlinear optical
properties of these species were investigated over the visible and
near-IR range, a particular emphasis being placed on their multiphoton
absorption properties; the complexes are shown to function as redox-switchable
nonlinear chromophores at selected wavelengths, and the more extended
derivatives are shown to exhibit the more promising NLO performance