3 research outputs found
Two Dynamic ABW-Type Metal Organic Frameworks Built of Pentacarboxylate and Zn<sup>2+</sup> as Photoluminescent Probes of Nitroaromatics
Self-assembly
reactions of Zn<sup>2+</sup> and L<sup>5ā</sup> (H<sub>5</sub>L = 2,5-(6-(4-carboxyphenylamino)-1,3,5-triazine-2,4-diyldiimino)
diterephthalic acid) lead to the formation of two new ABW-type zeolitic
metalāorganic frameworks (Z-MOFs): (Me<sub>2</sub>NH<sub>2</sub>)Ā[Zn<sub>2</sub>L]ĀĀ·3.5DMF (<b>1</b>) and (Me<sub>2</sub>NH<sub>2</sub>)Ā[Zn<sub>2</sub>LĀ(H<sub>2</sub>O)]ĀĀ·2DMFĀĀ·8H<sub>2</sub>O (<b>2</b>) (DMF = <i>N</i>,<i>N</i>-dimethylformamide). They are the first two Z-MOFs which are built
of the same pentacarboxylate ligand and metal ion but have two configurations
and channel shapes (distorted honeycomb- and herringbone-shaped channels
for <b>1</b> and <b>2</b> respectively). They can demonstrate
interesting structural transformations triggered by vacuum heating
or soaking in different solvents. While direct transformations between <b>1</b> and <b>2</b> were revealed to be not feasible, <b>2</b> could be first transformed to a crystalline intermediate <b>3</b> and then into <b>1</b>. Furthermore, while transformations
between <b>2</b> and <b>3</b> are irreversible, those
between <b>1</b> and <b>3</b> are reversible, accompanied
by a 26 nm shift of their emission peak positions. In comparison to
the ligand, <b>1</b>, <b>2</b>, and <b>3</b> exhibit
blue shifts in their luminescent emission peaks and have intensive
blue emission in both solid and solution phases. The efficient and
selective quenching of their photoluminescence by a series of nitroaromatics
(NACs) solutions phase and by nitrobenzene (NB) vapor makes them promising
probes for detecting NACs. <b>1</b>ā<b>3</b> represent
the first series of MOFs as promising photoluminescent probes for
detecting dinoseb down to 2.4 ppm. The electron transfer, long-range
energy transfer, and/or electrostatic interactions between the frameworks
and NACs mainly contribute to the quenching mechanisms
Optimizing Height and Packing Density of Oriented One-Dimensional Photocatalysts for Efficient Water Photoelectrolysis
Dependences of water-photoelectrolysis
efficiency on heights and
packing densities of vertically arrayed ZnO nanorods (NRs) and ZnO
microrods (MRs) were systematically studied for the first time over
a wide range of light incidence angles, under the direction of nanooptics
simulation. In the photoelectrolysis, dense NRs of 1.8 Ī¼m in
height afforded the highest photocatalytic efficiencies, and further
increases of the height kept lowering down the photocatalytic efficiencies,
while sparse MRs taller in height consistently afforded better electrolyte
penetration and higher photocurrent densities especially at higher
angles of incident light. The experimental results are in line with
the nanooptics simulation. This new finding is generally applicable
to advancing solar-energy conversions, optics, and optoelectronics
using oriented one-dimensional micro/nanocrystallites
1āD āPlatinum Wireā Stacking Structure Built of Platinum(II) Diimine Bis(Ļ-acetylide) Units with Luminescence in the NIR Region
A square-planar
platinumĀ(II) complex, PtĀ(DiBrbpy)Ā(Cī¼CC<sub>6</sub>H<sub>4</sub>Et-4)<sub>2</sub> (<b>1</b>) (DiBrbpy = 4,4-dibromo-2,2ā²-bipyridine),
and crystals of its three solvated forms, namely, <b>1</b>Ā·DMSO, <b>1</b>Ā·1/2Ā(CH<sub>3</sub>CN), and <b>1</b>Ā·1/8Ā(CH<sub>2</sub>Cl<sub>2</sub>), were developed and characterized. <b>1</b>Ā·DMSO and <b>1</b>Ā·1/2Ā(CH<sub>3</sub>CN) contain
quasi-dimeric and dimeric structures with luminescence in the visible
range, whereas <b>1</b>Ā·1/8Ā(CH<sub>2</sub>Cl<sub>2</sub>) exhibits NIR luminescence at 1022 nm due to its intrinsic 1-D āplatinum
wireā stacking structure with strong PtāPt interactions. <b>1</b>Ā·1/8Ā(CH<sub>2</sub>Cl<sub>2</sub>) represents the first
compound based on platinumĀ(II) diimine bisĀ(Ļ-acetylide) molecular
units with the NIR luminescence beyond 1000 nm. <b>1</b> selectively
responds to DMSO and CH<sub>3</sub>CN by changing its color and luminescence
property and the three solvated forms can be reversibly converted
to each other upon exposure to corresponding solvent vapors. Their
desolvated forms, namely <b>1a</b>, <b>1b</b>, and <b>1c</b>, obtained after heating <b>1</b>Ā·DMSO, <b>1</b>Ā·1/2Ā(CH<sub>3</sub>CN), and <b>1</b>Ā·1/8Ā(CH<sub>2</sub>Cl<sub>2</sub>), respectively, can also be restored to the
original solvated forms upon exposure to corresponding solvent vapors. <b>1a</b> and <b>1b</b> emit NIR luminescence peaked at 998
and 1018 nm respectively, suggesting indirect synthetic methods as
powerful alternatives to achieve NIR luminescence with long wavelength.
In contrast, <b>1c</b> exhibits a red luminescence with a broad
unstructured emission band centered at 667 nm. All the responses to
organic solvent vapors and heating are due to the structural transformations
which result in the conversion of the lowest energy excited states
between <sup>3</sup>MLCT/<sup>3</sup>LLCT and <sup>3</sup>MMLCT in
solid-state as supported by time-dependent density functional theory
(TD-DFT) calculations