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>

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    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

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    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

    No full text
    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

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    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

    No full text
    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
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