9 research outputs found
Stepwise Host–Guest [2 + 2] Photoreaction in a Hydrogen-Bonded One-Dimensional Coordination Polymer to a Two-Dimensional Layered Structure
Two hydrogen-bonded interdigitated
one-dimensional (1D) coordination
polymers (CPs) were synthesized from CdÂ(II) nitrate and 1,4-benzenedicarboxylate
(bdc) with two 4-styrylpyridine (4spy) derivatives. In the solid state
structure of 1D CP containing 2′-fluorostyrylpyridine (2F-4spy),
a guest 2F-4spy was sandwiched between the terminal 2F-4spy ligands
and the CC bonds of all the 2F-4spy are well-aligned in <i>host–guest-host–host-guest–host</i>- sequence
infinitely. From time-dependent photoreaction studies, it has been
found that the [2 + 2] photocycloaddition occurs between <i>host–guest</i> molecules first followed by <i>host–host</i> pairs
in a two-step process, which resulted in the quantitative conversion
of Cî—»C bond pairs to cyclobutane rings. It is a rare quantitative
photoreaction between the <i>host</i> and <i>guest</i> molecules. Further, solvothermal crystallization of the final photoproduct
furnished an interesting three-dimensional CP with <b>bcg</b> topology. Interestingly, 2NO<sub>2</sub>-4spy also furnished a similar
hydrogen-bonded 1D CP with parallel orientation of olefin bonds. Although
the olefin bonds satisfy the Schmidt’s criteria for photoreactivity,
it was found to be photoinert under UV light. This has been attributed
to the steric hindrance caused by NO<sub>2</sub> substituent or the
electron withdrawing effect
Influence of Fluorine Substitution on the Unusual Solid-State [2 + 2] Photo-Cycloaddition Reaction between an Olefin and an Aromatic Ring
Solid-state
[2 + 2] photo-cycloaddition reactions observed so far
were exclusively between a pair of olefin bonds. Usually when the
phenyl–olefin bonds have been closely aligned, they were found
to be either photoinert or sliding of molecules takes place for [2
+ 2] cycloaddition reaction between olefins in the solid state, although
intramolecular phenyl–olefin reactions are well-known in solution.
In the crystal structure of [Zn<sub>2</sub>(ptol)<sub>4</sub>Â(4spy)<sub>2</sub>] (ptol = <i>para</i>-toluate), the neighboring
4-styrylpyridine (4spy) ligands are organized in a head-to-tail manner.
On one side of the complex in the crystal structure, the olefin bonds
in the 4spy pairs are perfectly aligned to undergo cycloaddition reaction,
but on the other side, the olefin bond pairs are slightly offset and
found to be photoinert at 223 K forming only a dimer in single crystals.
The sliding of 4spy groups has been restricted by the steric hindrance
of the adjacent methyl group of the ptol ligands. A similar packing
of 2-fluoro-4′-styrylpyridine (2F-4spy) pairs was found in
[Zn<sub>2</sub>(ptol)<sub>4</sub>Â(2F-4spy)<sub>2</sub>]. Again,
normal cycloaddition reaction occurs on one side of the 2F-4spy ligand
pairs, whereas the second offset 2F-4spy ligand pairs undergo a rare
[2 + 2] cycloaddition reaction between the fluorophenyl group and
olefin bond resulting in the formation of a one-dimensional coordination
polymers containing a bicyclic product in a quantitative yield. The
bicyclic ring in the photoproduct can be thermally cleaved back to
olefin and phenyl groups. These observations have been confirmed by
single-crystal X-ray crystallography, <sup>1</sup>H NMR, and <sup>19</sup>F NMR studies. Density functional theory calculations were
performed to elucidate the nature of the interactions between the
fluorophenyl and olefin groups. The greater reduction of aromaticity
of 2F-4spy in the excited singlet state compared to the 4spy system
may explain the observed reactivity difference between the two systems.
The improved reactivity in 2F-4spy may also be attributed to the fact
that the olefin–phenyl distance is shorter in 2F-4spy than
in 4spy (3.63 versus 3.69 Å). This solid state phenyl–olefin
photodimerization helps to pave the way for making new bicyclic derivatives
Photosalient Behavior of Photoreactive Crystals
Being documented with only about
a dozen serendipitous observations,
the photosalient effect, where crystals leap when exposed to light,
is considered a very rare phenomenon. Here, with a set of structurally
related materials that undergo [2 + 2] photocycloaddition we present
evidence that this effect is more common than it has been realized
in the past, and we seek to establish correlations with the kinematics
and the crystal structure toward rational design of photosalient materials.
To that end, nine photoreactive complexes AgL<sub>2</sub>X<sub>2</sub> (L = 4-styrylpyridine, 2′-fluoro-4-styrylpyridine, and 3′-fluoro-4-styrylpyridine,
X = BF<sub>4</sub><sup>–</sup>, ClO<sub>4</sub><sup>–</sup> and NO<sub>3</sub><sup>–</sup>) were prepared. The [AgL<sub>2</sub>]<sup>+</sup> cations in these structures pack by both head-to-head
and head-to-tail alignment of the styrylpyridine ligands. Crystals
of six out of the nine complexes were photosalient and popped, hopped,
and/or leaped when exposed to UV light. It is concluded that the occurrence
of the photosalient effect is determined not only by the nature of
the ligand but also by the crystal packing which directs the magnitude,
direction, and rate of volume expansion during the photoreaction
Fabrication of Gold/Titania Photocatalyst for CO<sub>2</sub> Reduction Based on Pyrolytic Conversion of the Metal–Organic Framework NH<sub>2</sub>‑MIL-125(Ti) Loaded with Gold Nanoparticles
Titania exhibits unique photophysical
and -chemical properties
and can be used for potential applications in the field of photocatalysis.
The control of TiO<sub>2</sub> in terms of phase, shape, morphology,
and especially nanoscale synthesis of TiO<sub>2</sub> particles still
remains a challenge. Ti-containing metal–organic frameworks
(MOFs), such as MIL-125, can be used as sacrificial precursors to
obtain TiO<sub>2</sub> materials with diverse phase compositions,
morphologies, sizes, and surface areas. MIL-125 is composed of Ti/O
clusters as the secondary building units (SBUs) bridged by 1,4-benzenedicarboxylate
(bdc). In this study, preformed and surfactant-stabilized gold nanoparticles
(GNPs) were deposited onto the surface of amino functionalized NH<sub>2</sub>-MIL-125 during solvothermal synthesis. Targeted gold/titania
nanocomposites, GNP/TiO<sub>2</sub>, were fabricated through the pyrolysis
of GNP/NH<sub>2</sub>-MIL-125 nanocrystals. The modification of TiO<sub>2</sub> with GNPs significantly increased the photocatalytic activity
of the MOF derived TiO<sub>2</sub> material for the reduction of CO<sub>2</sub> to CH<sub>4</sub> as compared to TiO<sub>2</sub> reference
samples such as P-25 and AUROlite (Au/TiO<sub>2</sub>). The new materials
GNP/TiO<sub>2</sub> and TiO<sub>2</sub> derived by the MOF precursor
route were thoroughly characterized by PXRD, FTIR and Raman, TEM,
and N<sub>2</sub> adsorption studies
Solvent-Induced Structural Dynamics in Noninterpenetrating Porous Coordination Polymeric Networks
Three
novel soft porous coordination polymer (PCP) or metal–organic
framework (MOF) compounds have been synthesized with a new rigid ligand <i>N</i>-(4-pyridyl)-1,4,5,8-naphathalenetetracarboxymonoimide
(PNMI) by partial hydrolysis of <i>N,N′</i>-di-(4-pyridyl)-1,4,5,8-naphthalenete-tracarboxydiimide
(DPNI) during solvothermal reactions with ZnÂ(II), CdÂ(II), and MnÂ(II)
salts, and they are [ZnÂ(PNMI)]·2DMA (<b>1</b>·2DMA, <b>1a</b>), [CdÂ(PNMI)]·0.5DMA·5H<sub>2</sub>O (<b>2</b>·0.5DMA·5H<sub>2</sub>O), and [MnÂ(PNMI)]·0.75DMF (<b>3</b>·0.75DMF). The structure of <b>1</b> is based
on paddle-wheel secondary building unit (SBU) with a 3,6-connected <b>rtl</b> net topology, whereas <b>2</b> and <b>3</b> are isotypical but the MÂ(O<sub>2</sub>C–C)<sub>2</sub> fragments
aggregate in one-dimension and the overall connectivity is the same <b>rtl</b> net topology. All these three MOFs have one-dimensional
rhombic channels filled with guest molecules. The guest molecules
in <b>1a</b> can be exchanged with EtOH in a single-crystal
to single-crystal (SCSC) manner to <b>1</b>·1.25EtOH·0.375H<sub>2</sub>O (<b>1b</b>). Further, the guest molecules in <b>1b</b> can be replaced with ethylene glycol, triethylene glycol
and allyl alcohol without destroying its single crystal nature. These
guest exchanges are accompanied by reduction in volume of the unit
cell up to 16%, as well as the void volume up to 33.1%. Similarly,
triethylene glycol (TEGly) selectively exchanges EtOH in a mixture
of the above solvents, which might be the result of correct fit of
the hydrogen-bonded TEGly dimer in the channel of <b>1</b>.
While activated <b>1</b> and <b>3</b> exhibit no uptake
of N<sub>2</sub> and H<sub>2</sub> at 1 bar and 77 K and very low
uptake of CO<sub>2</sub> gas at 1 bar and 196 K, activated <b>2</b> shows selective CO<sub>2</sub> uptake, 278 cm<sup>2</sup>·g<sup>–1</sup>, over N<sub>2</sub> and H<sub>2</sub> at 1 bar and
196 K, which corresponds to 5.87 molecules of CO<sub>2</sub> per formula
unit of <b>2</b>
Influence of Angular Dicarboxylate Ligand on the Structures of Single and Double Pillared-Layer Coordination Polymers of Co(II)
Two pillared-layer coordination polymeric
compounds, namely, [Co<sub>2</sub>(bpeb)<sub>2</sub>(obc)<sub>2</sub>]·DMF·5H<sub>2</sub>O (<b>1</b>) and [Co<sub>2</sub>(bpeb)Â(obc)<sub>2</sub>]·2DMF·H<sub>2</sub>O (<b>2</b>), have been synthesized
using a long dipyridyl spacer ligand (1,4-bisÂ[2-(4-pyridyl)Âethenyl]Âbenzene,
bpeb), 4,4′-oxybisbenzoate (obc), and CoÂ(NO<sub>3</sub>)<sub>2</sub>·6H<sub>2</sub>O under solvothermal conditions, using
appropriate ratios of CoÂ(II) to bpeb. In compound <b>1</b>,
the double pillared-layer structure has a dimeric repeating unit and
exhibits <b>rob</b> topology, while single pillared-layer compound <b>2</b> has an unusual building block which is a linkage isomer
of the well-known paddle-wheel structure and has a <b>pcu</b> topology. Twofold and threefold interpenetrations are observed in <b>1</b> and <b>2</b>, respectively. The variable-temperature
magnetic properties of <b>1</b> and <b>2</b> were also
investigated. The double pillared-layer structure of <b>1</b> exhibits antiferromagnetic behavior while a relatively rare ferromagnetism
has been observed for the single pillared-layer structure of <b>2</b>
Influence of Angular Dicarboxylate Ligand on the Structures of Single and Double Pillared-Layer Coordination Polymers of Co(II)
Two pillared-layer coordination polymeric
compounds, namely, [Co<sub>2</sub>(bpeb)<sub>2</sub>(obc)<sub>2</sub>]·DMF·5H<sub>2</sub>O (<b>1</b>) and [Co<sub>2</sub>(bpeb)Â(obc)<sub>2</sub>]·2DMF·H<sub>2</sub>O (<b>2</b>), have been synthesized
using a long dipyridyl spacer ligand (1,4-bisÂ[2-(4-pyridyl)Âethenyl]Âbenzene,
bpeb), 4,4′-oxybisbenzoate (obc), and CoÂ(NO<sub>3</sub>)<sub>2</sub>·6H<sub>2</sub>O under solvothermal conditions, using
appropriate ratios of CoÂ(II) to bpeb. In compound <b>1</b>,
the double pillared-layer structure has a dimeric repeating unit and
exhibits <b>rob</b> topology, while single pillared-layer compound <b>2</b> has an unusual building block which is a linkage isomer
of the well-known paddle-wheel structure and has a <b>pcu</b> topology. Twofold and threefold interpenetrations are observed in <b>1</b> and <b>2</b>, respectively. The variable-temperature
magnetic properties of <b>1</b> and <b>2</b> were also
investigated. The double pillared-layer structure of <b>1</b> exhibits antiferromagnetic behavior while a relatively rare ferromagnetism
has been observed for the single pillared-layer structure of <b>2</b>
Regulating photosalient behavior in dynamic metal-organic crystals
Dynamic photoactuating crystals have become a sensation due to their potential applications in developing smart medical devices, molecular machines, artificial muscles, flexible electronics actuators, probes and microrobots. Here we report the synthesis of two iso-structural metal-organic crystals, [Zn(4-ohbz)2(4-nvp)2] (1) and [Cd(4-ohbz)2(4-nvp)2] (2) {H4-ohbz = 4-hydroxy benzoic acid; 4-nvp = 4-(1-naphthylvinyl)pyridine} which undergo topochemical [2 + 2] cycloaddition under UV irradiation as well as sunlight to generate a dimerized product of discrete metal-complex [Zn(4-ohbz)2(rctt-4-pncb)] {rctt-4-pncb = 1,3-bis(4′-pyridyl)-2,4-bis(naphthyl)cyclobutane} (1′) and one-dimensional coordination polymer (1D CP) [Cd(4-ohbz)2(rctt-4-pncb)] (2′) respectively, in a single-crystal-to-single-crystal (SCSC) process. The Zn-based compound demonstrates photosalient behaviour, wherein crystals show jumping, splitting, rolling, and swelling upon UV irradiation. However, the Cd-based crystals do not show such behaviour maintaining the initial supramolecular packing and space group. Thus the photomechanical behaviour can be induced by choosing a suitable metal ion. The above findings are thoroughly validated by quantitative density functional theory (DFT) calculations which show that the Zn-based crystal shifts towards an orthorhombic structure to resolve the anisotropic UV-induced mechanical strain. Furthermore, the mechano-structure-property relationship has been established by complimentary nanoindentation measurements, which are in-line with the DFT-predicted single crystal values.</p
Influence of Angular Dicarboxylate Ligand on the Structures of Single and Double Pillared-Layer Coordination Polymers of Co(II)
Two pillared-layer coordination polymeric
compounds, namely, [Co<sub>2</sub>(bpeb)<sub>2</sub>(obc)<sub>2</sub>]·DMF·5H<sub>2</sub>O (<b>1</b>) and [Co<sub>2</sub>(bpeb)Â(obc)<sub>2</sub>]·2DMF·H<sub>2</sub>O (<b>2</b>), have been synthesized
using a long dipyridyl spacer ligand (1,4-bisÂ[2-(4-pyridyl)Âethenyl]Âbenzene,
bpeb), 4,4′-oxybisbenzoate (obc), and CoÂ(NO<sub>3</sub>)<sub>2</sub>·6H<sub>2</sub>O under solvothermal conditions, using
appropriate ratios of CoÂ(II) to bpeb. In compound <b>1</b>,
the double pillared-layer structure has a dimeric repeating unit and
exhibits <b>rob</b> topology, while single pillared-layer compound <b>2</b> has an unusual building block which is a linkage isomer
of the well-known paddle-wheel structure and has a <b>pcu</b> topology. Twofold and threefold interpenetrations are observed in <b>1</b> and <b>2</b>, respectively. The variable-temperature
magnetic properties of <b>1</b> and <b>2</b> were also
investigated. The double pillared-layer structure of <b>1</b> exhibits antiferromagnetic behavior while a relatively rare ferromagnetism
has been observed for the single pillared-layer structure of <b>2</b>