22 research outputs found
Synthesis, Characterization, and Photocatalytic Activity of Y‑Doped CeO<sub>2</sub> Nanorods
Yttrium-doped ceria (YDC) nanorods
were prepared by hydrothermal
synthesis and characterized using Raman, UV–vis, transmission
electron microscopy, scanning electron microscopy/energy-dispersive
X-ray spectroscopy, X-ray photoelectron spectroscopy, and X-ray powder
diffraction. The ceria nanorods showed an increase in the amount of
oxygen vacancies with an increase in the Y concentration. When the
doping level is <30%, the optical band gap of the doped ceria is
lower than that of pure ceria nanorods. At < 50% of Y doping, the
composite nanorods exhibited a higher photocatalytic activity for
the degradation of model organic dyes compared to the pure ceria at
room temperature, and the catalyst with 10% loading showed the maximum
photocatalytic efficiency. However, at 100 °C, the photocatalytic
activity significantly improved for all the nanorods with different
Y loadings, and the greatest improvement was obtained for the sample
with the highest number of oxygen vacancies
Luminescent Metal–Organic Framework for the Selective Detection of Aldehydes
The detection of toxic, hazardous chemical species is
an important
task because they pose serious risks to either the environment or
human health. Luminescent metal–organic frameworks (LMOFs)
as alternative sensors offer rapid and sensitive detection of chemical
species. Interactions between chemical species and LMOFs result in
changes in the photoluminescence (PL) profile of the LMOFs which can
be readily detected using a simple fluorometer. Herein, we report
the use of a robust, Zn-based LMOF, [Zn5(μ3-OH)2(adtb)2(H2O)5·5
DMA] (Zn-adtb, LMOF-341), for the selective detection of benzaldehyde.
Upon exposure to benzaldehyde, Zn-adtb experiences significant luminescent
quenching, as characterized through PL experiments. Photoluminescent
titration experiments reveal that LMOF-341 has a detection limit of
64 ppm and a Ksv value of 179 M–1 for benzaldehyde. Furthermore, we study the guest–host interactions
that occur between LMOF-341 and benzaldehyde through in situ Fourier
transform infrared and computational modeling employing density functional
theory. The results show that benzaldehyde interacts more strongly
with LMOF-341 compared to formaldehyde and propionaldehyde. Our combined
studies also reveal that the mechanism of luminescence quenching originates
from an electron-transfer process
Stability and Hydrolyzation of Metal Organic Frameworks with Paddle-Wheel SBUs upon Hydration
Instability of most prototypical metal organic frameworks
(MOFs)
in the presence of moisture is always a limitation for industrial
scale development. In this work, we examine the dissociation mechanism
of microporous paddle wheel frameworks MÂ(bdc)Â(ted)<sub>0.5</sub> [M
= Cu, Zn, Ni, Co; bdc = 1,4-benzenedicarboxylate; ted = triethylenediamine]
in controlled humidity environments. Combined in situ IR spectroscopy,
Raman, and Powder X-ray diffraction measurements show that the stability
and modification of isostructual MÂ(bdc)Â(ted)<sub>0.5</sub> compounds
upon exposure to water vapor critically depend on the central metal
ion. A hydrolysis reaction of water molecules with Cu–O–C
is observed in the case of CuÂ(bdc)Â(ted)<sub>0.5</sub>. Displacement
reactions of ted linkers by water molecules are identified with ZnÂ(bdc)Â(ted)<sub>0.5</sub> and CoÂ(bdc)Â(ted)<sub>0.5</sub>. In contrast,. NiÂ(bdc)Â(ted)<sub>0.5</sub> is less susceptible to reaction with water vapors than
the other three compounds. In addition, the condensation of water
vapors into the framework is necessary to initiate the dissociation
reaction. These findings, supported by supported by first principles
theoretical van der Waals density functional (vdW-DF) calculations
of overall reaction enthalpies, provide the necessary information
for determining operation conditions of this class of MOFs with paddle
wheel secondary building units and guidance for developing more robust
units
Selective, Sensitive, and Reversible Detection of Vapor-Phase High Explosives via Two-Dimensional Mapping: A New Strategy for MOF-Based Sensors
A new strategy has been developed
for the effective detection of
high explosives in vapor phase by fluorescent metal–organic
framework (MOF) sensors. Two structurally related and dynamic MOFs,
(Zn)<sub>2</sub>(ndc)<sub>2</sub>P·<i>x</i>G [ndc =
2,6-naphthalenedicarboxylate;
P =1,2-bisÂ(4-pyridyl)Âethane (bpe) or 1,2-bisÂ(4-pyridyl)Âethylene (bpee);
G = guest/solvent molecule], exhibit a two-dimensional signal response
toward analytes of interest in the vapor phase, including aromatic
and aliphatic high explosives (e.g., TNT and RDX). The interaction
between analytes and the MOF has been studied using in situ infrared
absorption spectroscopy and a DFT computational method
CO<sub>2</sub> capture by hybrid ultramicroporous TIFSIX-3-Ni under humid conditions using non-equilibrium cycling
Although pyrazine-linked hybrid ultramicroporous materials (HUMs, pore size <7 Å) are benchmark physisorbents for trace carbon dioxide (CO2) capture under dry conditions, their affinity for water (H2O) mitigates their carbon capture performance in humid conditions. Herein, we report on the co-adsorption of H2O and CO2 by TIFSIX-3- Ni—a high CO2 affinity HUM—and find that slow H2O sorption kinetics can enable CO2 uptake and release using shortened adsorption cycles with retention of ca. 90% of dry CO2 uptake. Insight into co-adsorption is provided by in situ infrared spectroscopy and ab initio calculations. The binding sites and sorption mechanisms reveal that both CO2 and H2O molecules occupy the same ultramicropore through favorable interactions between CO2 and H2O at low water loading. An energetically favored water network displaces CO2 molecules at higher loading. Our results offer bottom-up design principles and insight into co-adsorption of CO2 and H2O that is likely to be relevant across the full spectrum of carbon capture sorbents to better understand and address the challenge posed by humidity to gas capture.</p
Competitive Coadsorption of CO<sub>2</sub> with H<sub>2</sub>O, NH<sub>3</sub>, SO<sub>2</sub>, NO, NO<sub>2</sub>, N<sub>2</sub>, O<sub>2</sub>, and CH<sub>4</sub> in M‑MOF-74 (M = Mg, Co, Ni): The Role of Hydrogen Bonding
The importance of coadsorption for
applications of porous materials
in gas separation has motivated fundamental studies, which have initially
focused on the comparison of the binding energies of different gas
molecules in the pores (i.e., energetics) and their overall transport.
By examining the competitive coadsorption of several small molecules
in M-MOF-74 (M = Mg, Co, Ni) with in situ infrared spectroscopy and
ab initio simulations, we find that the binding energy at the most
favorable (metal) site is not a sufficient indicator for prediction
of molecular adsorption and stability in MOFs. Instead, the occupation
of the open metal sites is governed by kinetics, whereby the interaction
of the guest molecules with the MOF organic linkers controls the reaction
barrier for molecular exchange. Specifically, the displacement of
CO<sub>2</sub> adsorbed at the metal center by other molecules such
as H<sub>2</sub>O, NH<sub>3</sub>, SO<sub>2</sub>, NO, NO<sub>2</sub>, N<sub>2</sub>, O<sub>2</sub>, and CH<sub>4</sub> is mainly observed
for H<sub>2</sub>O and NH<sub>3</sub>, even though SO<sub>2</sub>,
NO, and NO<sub>2</sub> have higher binding energies (∼70–90
kJ/mol) to metal sites than that of CO<sub>2</sub> (38 to 48 kJ/mol)
and slightly higher than that of water (∼60–80 kJ/mol).
DFT simulations evaluate the barriers for H<sub>2</sub>O →
CO<sub>2</sub> and SO<sub>2</sub> → CO<sub>2</sub> exchange
to be ∼13 and 20 kJ/mol, respectively, explaining the slow
exchange of CO<sub>2</sub> by SO<sub>2</sub>, compared to water. Furthermore,
the calculations reveal that the kinetic barrier for this exchange
is determined by the specifics of the interaction of the second guest
molecule (e.g., H<sub>2</sub>O or SO<sub>2</sub>) with the MOF ligands.
Hydrogen bonding of H<sub>2</sub>O molecules with the nearby oxygen
of the organic linker is found to facilitate the positioning of the
H<sub>2</sub>O oxygen atom toward the metal center, thus reducing
the exchange barrier. In contrast, SO<sub>2</sub> molecules interact
with the distant benzene site, away from the metal center, hindering
the exchange process. Similar considerations apply to the other molecules,
accounting for much easier CO<sub>2</sub> exchange for NH<sub>3</sub> than for NO, NO<sub>2</sub>, CH<sub>4</sub>, O<sub>2</sub>, and
N<sub>2</sub> molecules. In this work, critical parameters such as
kinetic barrier and exchange pathway are first unveiled and provide
insight into the mechanism of competitive coadsorption, underscoring
the need of combined studies, using spectroscopic methods and ab initio
simulations to uncover the atomistic interactions of small molecules
in MOFs that directly influence coadsorption
Water Reaction Mechanism in Metal Organic Frameworks with Coordinatively Unsaturated Metal Ions: MOF-74
Water dissociation represents one
of the most important reactions
in catalysis, essential to the surface and nano sciences [e.g., Hass et al., Science, 1998 282, 265–268; Brown et al., Science, 2001, 294, 67–69; Bikondoa et al., Nature, 2005, 5, 189–192]. However, the dissociation
mechanism on most oxide surfaces is not well understood due to the
experimental challenges of preparing surface structures and characterizing
reaction pathways. To remedy this problem, we propose the metal organic
framework MOF-74 as an ideal model system to study water reactions.
Its crystalline structure is well characterized; the metal oxide node
mimics surfaces with exposed cations; and it degrades in water. Combining <i>in situ</i> IR spectroscopy and first-principles calculations,
we explored the MOF-74/water interaction as a function of vapor pressure
and temperature. Here, we show that, while adsorption is reversible
below the water condensation pressure (∼19.7 Torr) at room
temperature, a reaction takes place at ∼150 °C even at
low water vapor pressures. This important finding is unambiguously
demonstrated by a clear spectroscopic signature of the direct reaction
using D<sub>2</sub>O, which is not present using H<sub>2</sub>O due
to strong phonon coupling. Specifically, a sharp absorption band appears
at 970 cm<sup>–1</sup> when D<sub>2</sub>O is introduced at
above 150 °C, which we attribute to an O–D bending vibration
on the phenolate linker. Although H<sub>2</sub>O undergoes a similar
dissociation reaction, the corresponding O–H mode is too strongly
coupled to MOF vibrations to detect. In contrast, the O–D mode
falls in the phonon gap of the MOF and remains localized. First-principles
calculations not only positively identify the O–D mode at 970
cm<sup>–1</sup> but derive a pathway and kinetic barrier for
the reaction and the final configuration: the D (H) atom is transferred
to the oxygen of the linker phenolate group, producing the notable
O–D absorption band at 970 cm<sup>–1</sup>, while the
OD (or OH) binds to the open metal sites. This finding explains water
dissociation in this case and provides insight into the long-lasting
question of MOF-74 degradation. Overall, it adds to the understanding
of molecular water interaction with cation-exposed surfaces to enable
development of more efficient catalysts for water dissociation
Modulation of water vapor sorption by a 4th generation metal-organic material with a rigid framework and self-switching pores
Hydrolytically stable adsorbents are needed for water vapor sorption related applications; however, design principles for porous materials with tunable water sorption behavior are not yet established. Here, we report that a platform of fourth-generation metal–organic materials (MOMs) with rigid frameworks and self-switching pores can adapt their pores to modulate water sorption. This platform is based upon the hydrolytically stable material CMOM-3S, which exhibits bnn topology and is composed of rod building blocks based upon S-mandelate ligands, 4,4-bipyridine ligands, and extraframework triflate anions. Isostructural variants of CMOM-3S were prepared using substituted R-mandelate ligands and exhibit diverse water vapor uptakes (20–67 cm3/g) and pore filling pressures (P/P0, 0.55–0.75). [Co2(R-4-Cl-man)2(bpy)3](OTf) (33R) is of particular interest because of its unusual isotherm. Insight into the different water sorption properties of the materials studied was gained from analysis of in situ vibrational spectra, which indicate self-switching pores via perturbation of extraframework triflate anions and mandelate linker ligands to generate distinctive water binding sites. Water vapor adsorption was studied using in situ differential spectra that reveal gradual singlet water occupancy followed by aggregation of water clusters in the channels upon increasing pressure. First-principles calculations identified the water binding sites and provide structural insight on how adsorbed water molecules affect the structures and the binding sites. Stronger triflate hydrogen bonding to the framework along with significant charge redistribution were determined for water binding in 33R. This study provides insight into a new class of fourth-generation (self-switching pores) MOM and the resulting effect upon water vapor sorption propertie
Mechanism of Preferential Adsorption of SO<sub>2</sub> into Two Microporous Paddle Wheel Frameworks M(bdc)(ted)<sub>0.5</sub>
The
selective adsorption of a corrosive gas, SO<sub>2</sub>, into
two microporous pillared paddle-wheel frameworks MÂ(bdc)Â(ted)<sub>0.5</sub> [<i>M</i> = Ni, Zn; bdc =1,4-benzenedicarboxylate; ted
= triethylenediamine] is studied by volumetric adsorption measurements
and a combination of <i>in situ</i> infrared spectroscopy
and <i>ab initio</i> density functional theory (DFT) calculations.
The uptake of SO<sub>2</sub> in MÂ(bdc)Â(ted)<sub>0.5</sub> at room
temperature is quite significant, 9.97 mol/kg at 1.13 bar. The major
adsorbed SO<sub>2</sub> molecules contributing to the isotherm measurements
are characterized by stretching bands at 1326 and 1144 cm<sup>–1</sup>. Theoretical calculations including van der Waals interactions (based
on vdW-DF) suggest that two adsorption configurations are possible
for these SO<sub>2</sub> molecules. One geometry involves an SO<sub>2</sub> molecule bonded through its sulfur atom to the oxygen atom
of the paddle-wheel building unit and its two oxygen atoms to the
C–H groups of the organic linkers by formation of hydrogen
bonds. Such a configuration results in a distortion of the benzene
rings, which is consistent with the experimentally observed shift
of the ring deformation mode. In the other geometry, SO<sub>2</sub> establishes hydrogen bonding with −CH<sub>2</sub> group of
the ted linker through its two oxygen atoms simultaneously. The vdW-DF-simulated
frequency shifts of the SO<sub>2</sub> stretching bands in these two
configurations are similar and in good agreement with spectroscopically
measured values of physisorbed SO<sub>2</sub>. In addition, the IR
spectra reveal the presence of another minor species, characterized
by stretching modes at 1242 and 1105 cm<sup>–1</sup> and causing
significant perturbations of MOFs vibrational modes (CH<sub><i>x</i></sub> and carboxylate groups). This species is more strongly
bound, requiring a higher temperature (∼150 °C) to remove
it than for the main physisorbed species. The adsorption configurations
of SO<sub>2</sub> into MÂ(bdc)Â(ted)<sub>0.5</sub> derived by infrared
spectroscopy and vdW-DF calculations provide the initial understanding
to develop microporous metal organic frameworks materials based on
paddlewheel secondary-building units for SO<sub>2</sub> removal in
industrial processes