5 research outputs found
Topological Analysis of Void Spaces in Tungstate Frameworks: Assessing Storage Properties for the Environmentally Important Guest Molecules and Ions: CO<sub>2</sub>, UO<sub>2</sub>, PuO<sub>2</sub>, U, Pu, Sr<sup>2+</sup>, Cs<sup>+</sup>, CH<sub>4</sub>, and H<sub>2</sub>
The identification of inorganic materials,
which are able to encapsulate
environmentally important small molecules or ions via host–guest
interactions, is crucial for the design and development of next-generation
energy sources and for storing environmental waste. Especially sought
after are molecular sponges with the ability to incorporate CO<sub>2</sub>, gas pollutants, or nuclear waste materials such as UO<sub>2</sub> and PuO<sub>2</sub> oxides or U, Pu, Sr<sup>2+</sup>, or
Cs<sup>+</sup> ions. Porous framework structures promise very attractive
prospects for applications in environmental technologies, if they
are able to incorporate CH<sub>4</sub> for biogas energy applications
or to store H<sub>2</sub>, which is important for fuel cells, e.g.,
in the automotive industry. All of these applications should benefit
from the host being resistant to extreme conditions such as heat,
nuclear radiation, rapid gas expansion, or wear and tear from heavy
gas cycling. As inorganic tungstates are well known for their thermal
stability and their rigid open-framework networks, the potential of
Na<sub>2</sub>O–Al<sub>2</sub>O<sub>3</sub>–WO<sub>3</sub> and Na<sub>2</sub>O–WO<sub>3</sub> phases for such applications
was evaluated. To this end, all known experimentally determined crystal
structures with the stoichiometric formula M<sub>a</sub>M′<sub>b</sub>W<sub>c</sub>O<sub>d</sub> (M = any element) are surveyed
together with all corresponding theoretically calculated Na<sub>a</sub>Al<sub>b</sub>W<sub>c</sub>O<sub>d</sub> and Na<sub><i>x</i></sub>W<sub><i>y</i></sub>O<sub><i>z</i></sub> structures that are statistically likely to form. Network descriptors
that categorize these host structures are used to reveal topological
patterns in the hosts, including the nature of porous cages, which
are able to accommodate a certain type of guest; this leads to the
classification of preferential structure types for a given environmental
storage application. Crystal structures of two new tungstates NaAlW<sub>2</sub>O<sub>8</sub> (<b>1</b>) and NaAlW<sub>3</sub>O<sub>11</sub> (<b>2</b>) and one updated structure determination
of Na<sub>2</sub>W<sub>2</sub>O<sub>7</sub> (<b>3</b>) are also
presented from in-house X-ray diffraction studies, and their potential
merits for environmental applications are assessed against those of
this larger data-sourced survey. Overall, results show that tungstate
structures with three-nodal topologies are most frequently able to
accommodate CH<sub>4</sub> or H<sub>2</sub>, while CO<sub>2</sub> appears
to be captured by a wide range of nodal structure types. The computationally
generated host structures appear systematically smaller than the experimentally
determined structures. For the structures of <b>1</b> and <b>2</b>, potential applications in nuclear waste storage seem feasible
Molecular Origins of Optoelectronic Properties in Coumarin Dyes: Toward Designer Solar Cell and Laser Applications
Coumarin derivatives are used in a wide range of applications, such as dye-sensitized solar cells (DSCs) and dye lasers, and have therefore attracted considerable research interest. In order to understand the molecular origins of their optoelectronic properties, molecular structures for 29 coumarin laser dyes are statistically analyzed. To this end, data for 25 compounds were taken from the Cambridge Structural Database and compared with data for four new crystal structures of coumarin laser dyes [Coumarin 487 (C<sub>19</sub>H<sub>23</sub>NO<sub>2</sub>), Coumarin 498 (C<sub>16</sub>H<sub>17</sub>NO<sub>4</sub>S), Coumarin 510 (C<sub>20</sub>H<sub>18</sub>N<sub>2</sub>O<sub>2</sub>), and Coumarin 525 (C<sub>22</sub>H<sub>18</sub>N<sub>2</sub>O<sub>3</sub>)], which are reported herein. The competing contributions of different resonance states to the bond lengths of the 4- and 7-substituted coumarin laser dyes are computed based on the harmonic oscillator stabilization energy model. Consequently, a positive correlation between the contribution of the <i>para</i>-quinoidal resonance state and the UV–vis peak absorption wavelength of these coumarins is revealed. Furthermore, the perturbations of optoelectronic properties, owing to chemical substituents in these coumarin laser dyes, are analyzed: it is found that their UV–vis peak absorption and lasing wavelengths experience a red shift, as the electron-donating strength of the 7-position substituent increases and/or the electron-withdrawing strength of the 3- or 4-position substituent rises; this conclusion is corroborated by quantum-chemical calculations. It is also revealed that the closer the relevant substituents align with the direction of the intramolecular charge transfer (ICT), the larger the spectral shifts and the higher the molar extinction coefficients of coumarin laser dyes. These findings are important for understanding the ICT mechanism in coumarins. Meanwhile, all structure–property correlations revealed herein will enable knowledge-based molecular design of coumarins for dye lasers and DSC applications
Molecular Origins of Optoelectronic Properties in Coumarin Dyes: Toward Designer Solar Cell and Laser Applications
Coumarin derivatives are used in a wide range of applications, such as dye-sensitized solar cells (DSCs) and dye lasers, and have therefore attracted considerable research interest. In order to understand the molecular origins of their optoelectronic properties, molecular structures for 29 coumarin laser dyes are statistically analyzed. To this end, data for 25 compounds were taken from the Cambridge Structural Database and compared with data for four new crystal structures of coumarin laser dyes [Coumarin 487 (C<sub>19</sub>H<sub>23</sub>NO<sub>2</sub>), Coumarin 498 (C<sub>16</sub>H<sub>17</sub>NO<sub>4</sub>S), Coumarin 510 (C<sub>20</sub>H<sub>18</sub>N<sub>2</sub>O<sub>2</sub>), and Coumarin 525 (C<sub>22</sub>H<sub>18</sub>N<sub>2</sub>O<sub>3</sub>)], which are reported herein. The competing contributions of different resonance states to the bond lengths of the 4- and 7-substituted coumarin laser dyes are computed based on the harmonic oscillator stabilization energy model. Consequently, a positive correlation between the contribution of the <i>para</i>-quinoidal resonance state and the UV–vis peak absorption wavelength of these coumarins is revealed. Furthermore, the perturbations of optoelectronic properties, owing to chemical substituents in these coumarin laser dyes, are analyzed: it is found that their UV–vis peak absorption and lasing wavelengths experience a red shift, as the electron-donating strength of the 7-position substituent increases and/or the electron-withdrawing strength of the 3- or 4-position substituent rises; this conclusion is corroborated by quantum-chemical calculations. It is also revealed that the closer the relevant substituents align with the direction of the intramolecular charge transfer (ICT), the larger the spectral shifts and the higher the molar extinction coefficients of coumarin laser dyes. These findings are important for understanding the ICT mechanism in coumarins. Meanwhile, all structure–property correlations revealed herein will enable knowledge-based molecular design of coumarins for dye lasers and DSC applications
Material Profiling for Photocrystallography: Relating Single-Crystal Photophysical and Structural Properties of Luminescent Bis-Cyclometalated Iridium-Based Complexes
The
photophysical properties of seven luminescent iridium complexes
are characterized in their single-crystal form, and the photoactivity
is related to their molecular structures. Specifically, solid-state
optical emission spectra and associated lifetimes are determined from
single crystals of iridium complexes containing three bidentate ligands:
two variously substituted 2-phenylbenzothiazoles and either a 2,4-pentadione
(acetylacetone) or 2-pyridinecarboxylic (picolinic) acid. All complexes
studied exhibit emissive behavior in the solid-state which originates
from <sup>3</sup>π–π* and metal-to-ligand-charge-transfer
(MLCT) electronic transitions; this is supported by density functional
theory. Phosphorescence is observed in all cases with microsecond
lifetimes, ranging from 0.30 to 2.4 μs at 298 K and 1.4–4.0
μs at 100 K. Structure–property relationships are established
which are relevant to the potential solid-state application of this
series of luminescent complexes as organic light emitting diodes (OLED)
material components. In addition, these materials are assessed for
their suitability to time-resolved pump–probe photocrystallography
experiments, which will reveal their photoexcited state structure.
Accordingly, the design process by which materials are selected and
technical parameters are defined for a photocrystallography experiment
is illustrated. This family of complexes presents a case study for
this photocrystallography material profiling. Results show that the
time-resolved photoexcited state structure, featuring the MLCT transition
is, in principle at least, viable for two of these complexes
Material Profiling for Photocrystallography: Relating Single-Crystal Photophysical and Structural Properties of Luminescent Bis-Cyclometalated Iridium-Based Complexes
The
photophysical properties of seven luminescent iridium complexes
are characterized in their single-crystal form, and the photoactivity
is related to their molecular structures. Specifically, solid-state
optical emission spectra and associated lifetimes are determined from
single crystals of iridium complexes containing three bidentate ligands:
two variously substituted 2-phenylbenzothiazoles and either a 2,4-pentadione
(acetylacetone) or 2-pyridinecarboxylic (picolinic) acid. All complexes
studied exhibit emissive behavior in the solid-state which originates
from <sup>3</sup>π–π* and metal-to-ligand-charge-transfer
(MLCT) electronic transitions; this is supported by density functional
theory. Phosphorescence is observed in all cases with microsecond
lifetimes, ranging from 0.30 to 2.4 μs at 298 K and 1.4–4.0
μs at 100 K. Structure–property relationships are established
which are relevant to the potential solid-state application of this
series of luminescent complexes as organic light emitting diodes (OLED)
material components. In addition, these materials are assessed for
their suitability to time-resolved pump–probe photocrystallography
experiments, which will reveal their photoexcited state structure.
Accordingly, the design process by which materials are selected and
technical parameters are defined for a photocrystallography experiment
is illustrated. This family of complexes presents a case study for
this photocrystallography material profiling. Results show that the
time-resolved photoexcited state structure, featuring the MLCT transition
is, in principle at least, viable for two of these complexes