14 research outputs found
<sup>25</sup>Mg Solid-State NMR: A Sensitive Probe of Adsorbing Guest Molecules on a Metal Center in Metal–Organic Framework CPO-27-Mg
Metal–organic frameworks (MOFs) have excellent
adsorption
capability. To understand their adsorptive properties requires detailed
information on the host–guest interaction. The information
on MOF desolvation (or activation) is also crucial because the very
first step of many applications requires removal of the solvent molecules
occluded inside of the pores. Unfortunately, such information is not
always available from powder XRD data. Solid-state NMR is an excellent
complementary technique to XRD. CPO-27-Mg is a MOF with unusual adsorption
ability. The adsorption involves a direct interaction between Mg and
guest species. Herein, we present, for the first time, a natural abundance <sup>25</sup>Mg solid-state NMR study of CPO-27-Mg at an ultrahigh magnetic
field of 21.1 T. The results provide new physical insights into the
effects of dehydration/rehydration and adsorption of guest species
on the Mg local environment
Chlorine-35 Solid-State NMR Spectroscopy as an Indirect Probe of Germanium Oxidation State and Coordination Environment in Germanium Chlorides
Due
to the prevalence of Ge–Cl bonds in germanium chemistry and
the inherent challenges of germanium-73 NMR spectroscopy, chlorine-35
NMR spectroscopy was investigated as an indirect method of characterization
for these ubiquitous and useful compounds. Chlorine-35 NMR parameters
were correlated with structural metrics as well as the oxidation state
of germanium
Mapping Out Chemically Similar, Crystallographically Nonequivalent Hydrogen Sites in Metal–Organic Frameworks by <sup>1</sup>H Solid-State NMR Spectroscopy
Metal–organic frameworks (MOFs) are important materials
with many actual and potential applications. Crystal structure of
many MOFs is determined by single-crystal X-ray diffraction. However,
due to the inability of XRD to accurately locate hydrogen atoms, the
local structures around framework hydrogen are usually poorly characterized
even if the overall framework has been accurately determined. <sup>1</sup>H solid-state NMR (SSNMR) spectroscopy should, in principle,
be used as a complementary method to XRD for characterizing hydrogen
local environments. However, the spectral resolution of <sup>1</sup>H SSNMR is severely limited by the strong <sup>1</sup>H–<sup>1</sup>H homonuclear dipolar coupling. In this work, we demonstrate
that high-resolution <sup>1</sup>H MAS spectra of MOF-based material
can be obtained by ultrafast sample spinning at high magnetic field
in combination with isotopic dilution. In particular, we examined
an important MOF, microporous α-Mg<sub>3</sub>(HCOO)<sub>6</sub> and α-Mg<sub>3</sub>(HCOO)<sub>6</sub> in the presence of
several guest species. All six chemically very similar, but crystallographically,
nonequivalent H sites of these MOFs were resolved in a chemical shift
range as small as 0.8 ppm. Although the assignment of <sup>1</sup>H peaks due to crystallographically nonequivalent hydrogens is difficult
due to that they all have almost identical chemical environments,
we are able to show that they can be assigned from <sup>1</sup>H–<sup>1</sup>H proximity maps obtained from 2D <sup>1</sup>H–<sup>1</sup>H double quantum (DQ) experiments in conjunction with theoretical
calculations. <sup>1</sup>H MAS spectra of framework hydrogen are
very sensitive to the guest molecules present inside the pores and
they provide insight into host–guest interaction and dynamics
of guest molecule. The ability of achieving very high resolution for <sup>1</sup>H MAS NMR in MOF-based materials and subsequent spectral assignment
demonstrated in this work allows one to obtain new structural information
complementary to that obtained from single-crystal XRD
Wobbling and Hopping: Studying Dynamics of CO<sub>2</sub> Adsorbed in Metal–Organic Frameworks via <sup>17</sup>O Solid-State NMR
Knowledge of adsorbed gas dynamics within microporous solids is crucial for the design of more efficient gas capture materials. We demonstrate that <sup>17</sup>O solid-state NMR (SSNMR) experiments allow one to obtain accurate information on CO<sub>2</sub> dynamics within metal–organic frameworks (MOFs), using CPO-27-M (M = Mg, Zn) as examples. Variable-temperature (VT) <sup>17</sup>O SSNMR spectra acquired from 150 to 403 K yield key parameters defining the CO<sub>2</sub> motions. VT <sup>17</sup>O SSNMR spectra of CPO-27-Zn indicate relatively weaker metal–oxygen binding and increased CO<sub>2</sub> dynamics. <sup>17</sup>O SSNMR is a sensitive probe of CO<sub>2</sub> dynamics due to the presence of both the quadrupolar and chemical shielding interactions, and holds potential for the investigation of motions within a variety of microporous materials
Solid-State <sup>63</sup>Cu, <sup>65</sup>Cu, and <sup>31</sup>P NMR Spectroscopy of Photoluminescent Copper(I) Triazole Phosphine Complexes
The
results of a solid-state <sup>63/65</sup>Cu and <sup>31</sup>P NMR
investigation of several copperÂ(I) complexes with functionalized
3-(2′-pyridyl)-1,2,4-triazole and phosphine ligands that have
shown potential in the preparation of photoluminescent devices are
reported. For each complex studied, distinct NMR parameters, with
moderate <sup>63</sup>Cu nuclear quadrupolar coupling constant (<i>C</i><sub>Q</sub>) values ranging from −17.2 to −23.7
MHz, are attributed to subtle variations in the distorted four-coordinate
environments about the copper nuclei. The spans of the copper chemical
shift (CS) tensors, δ<sub>11</sub>–δ<sub>33</sub>, for the mono- and bisphosphine complexes are also similar, ranging
from 1000 to 1150 ppm, but that for a complex with a strained bidentate
phosphine ligand is only 650 ppm. The effects of residual dipolar
and indirect spin–spin coupling arising from the <sup>63/65</sup>Cu– <sup>31</sup>P spin pairs, observed in the solid-state <sup>31</sup>P NMR spectra of these complexes, yield information about
the orientations of the copper electric field gradient (EFG) tensors
relative to the Cu–P bond. Variable-temperature <sup>31</sup>P NMR measurements for [CuÂ(bptzH)Â(dppe)]ÂClO<sub>4</sub> (bptzH
= 5-<i>tert</i>-butyl-3-(2′-pyridyl)-1,2,4-triazole;
dppe = 1,2-bisÂ(diphenylphosphino)Âethane), undertaken to investigate
the cause of the broad unresolved spectra observed at room temperature,
demonstrate that the broadening arises from partial self-decoupling
of the <sup>63/65</sup>Cu nuclei, a consequence of rapid quadrupolar
relaxation. Ab initio calculations of copper EFG and CS tensors were
performed to probe relationships between NMR parameters and molecular
structure. The analysis demonstrated that <i>C</i><sub>Q</sub>(<sup>63/65</sup>Cu) is negative for all complexes studied here
and that the largest components of the EFG tensors are generally coincident
with δ<sub>11</sub>
Experimental Characterization of the Hydride <sup>1</sup>H Shielding Tensors for HIrX<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub> and HRhCl<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub>: Extremely Shielded Hydride Protons with Unusually Large Magnetic Shielding Anisotropies
The
hydride proton magnetic shielding tensors for a series of iridiumÂ(III)
and rhodiumÂ(III) complexes are determined. Although it has long been
known that hydridic protons for transition-metal hydrides are often
extremely shielded, this is the first experimental determination of
the shielding tensors for such complexes. Isolating the <sup>1</sup>H NMR signal for a hydride proton requires careful experimental strategies
because the spectra are generally dominated by ligand <sup>1</sup>H signals. We show that this can be accomplished for complexes containing
as many as 66 ligand protons by substituting the latter with deuterium
and by using hyperbolic secant pulses to selectively irradiate the
hydride proton signal. We also demonstrate that the quality of the
results is improved by performing experiments at the highest practical
magnetic field (21.14 T for the work presented here). The hydride
protons for iridium hydride complexes HIrX<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub> (X = Cl, Br, or I; R = isopropyl, cyclohexyl) are highly
shielded with isotropic chemical shifts of approximately −50
ppm and are also highly anisotropic, with spans (=δ<sub>11</sub> – δ<sub>33</sub>) ranging from 85.1 to 110.7 ppm. The
hydridic protons for related rhodium complexes HRhCl<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub> also have unusual magnetic shielding properties
with chemical shifts and spans of approximately −32 and 85
ppm, respectively. Relativistic density functional theory computations
were performed to determine the orientation of the principal components
of the hydride proton shielding tensors and to provide insights into
the origin of these highly anisotropic shielding tensors. The results
of our computations agree well with experiment, and our conclusions
concerning the importance of relativistic effects support those recently
reported by Kaupp and co-workers
Experimental Characterization of the Hydride <sup>1</sup>H Shielding Tensors for HIrX<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub> and HRhCl<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub>: Extremely Shielded Hydride Protons with Unusually Large Magnetic Shielding Anisotropies
The
hydride proton magnetic shielding tensors for a series of iridiumÂ(III)
and rhodiumÂ(III) complexes are determined. Although it has long been
known that hydridic protons for transition-metal hydrides are often
extremely shielded, this is the first experimental determination of
the shielding tensors for such complexes. Isolating the <sup>1</sup>H NMR signal for a hydride proton requires careful experimental strategies
because the spectra are generally dominated by ligand <sup>1</sup>H signals. We show that this can be accomplished for complexes containing
as many as 66 ligand protons by substituting the latter with deuterium
and by using hyperbolic secant pulses to selectively irradiate the
hydride proton signal. We also demonstrate that the quality of the
results is improved by performing experiments at the highest practical
magnetic field (21.14 T for the work presented here). The hydride
protons for iridium hydride complexes HIrX<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub> (X = Cl, Br, or I; R = isopropyl, cyclohexyl) are highly
shielded with isotropic chemical shifts of approximately −50
ppm and are also highly anisotropic, with spans (=δ<sub>11</sub> – δ<sub>33</sub>) ranging from 85.1 to 110.7 ppm. The
hydridic protons for related rhodium complexes HRhCl<sub>2</sub>(PR<sub>3</sub>)<sub>2</sub> also have unusual magnetic shielding properties
with chemical shifts and spans of approximately −32 and 85
ppm, respectively. Relativistic density functional theory computations
were performed to determine the orientation of the principal components
of the hydride proton shielding tensors and to provide insights into
the origin of these highly anisotropic shielding tensors. The results
of our computations agree well with experiment, and our conclusions
concerning the importance of relativistic effects support those recently
reported by Kaupp and co-workers
Solid State Complex Chemistry: Formation, Structure, and Properties of Homoleptic Tetracyanamidogermanates RbRE[Ge(CN<sub>2</sub>)<sub>4</sub>] (RE = La, Pr, Nd, Gd)
Tetracyanamidometallates with the
general formula RbREÂ[TÂ(CN<sub>2</sub>)<sub>4</sub>] (RE = La, Pr,
Nd, Gd; T = Si, Ge) were prepared
by solid state metathesis reactions starting from stoichiometric mixtures
of RECl<sub>3</sub>, A<sub>2</sub>[TF<sub>6</sub>], and Li<sub>2</sub>(CN<sub>2</sub>). Reactions were studied by differential thermal
analysis that showed ignition temperatures between 360 and 390 °C
for the formation of RbGdÂ[TÂ(CN<sub>2</sub>)<sub>4</sub>] with T =
Si and Ge. The powder diffraction patterns of RbREÂ[GeÂ(CN<sub>2</sub>)<sub>4</sub>] were indexed isotypically to the already known RbREÂ[SiÂ(CN<sub>2</sub>)<sub>4</sub>] compound. IR spectra of RbLaÂ[GeÂ(CN<sub>2</sub>)<sub>4</sub>] were measured and compared with those of RbLaÂ[SiÂ(CN<sub>2</sub>)<sub>4</sub>]. <sup>73</sup>Ge, <sup>87</sup>Rb, and <sup>139</sup>La solid state NMR measurements and density functional theory
calculations were used to verify the novel homoleptic [GeÂ(CN<sub>2</sub>)<sub>4</sub>]<sup>4–</sup> ion. Luminescence properties of
Eu<sup>3+</sup>, Ce<sup>3+</sup>, and Tb<sup>3+</sup> doped samples
are reported
Cold, Hot, Dry, and Wet: Locations and Dynamics of CO<sub>2</sub> and H<sub>2</sub>O Co-Adsorbed in an Ultramicroporous MOF
Climate change from anthropogenic carbon dioxide (CO2) emissions poses a severe threat to society. A variety of
mitigation
strategies currently include some form of CO2 capture.
Metal–organic frameworks (MOFs) have shown great promise for
carbon capture and storage, but several issues must be solved before
feasible widespread adoption is possible. MOFs often exhibit reduced
chemical stabilities and CO2 adsorption capacities in the
presence of water, which is ubiquitous in nature and many practical
settings. A comprehensive understanding of water influence on CO2 adsorption in MOFs is necessary. We have used multinuclear
nuclear magnetic resonance (NMR) experiments at temperatures ranging
from 173 to 373 K, along with complementary computational techniques,
to investigate the co-adsorption of CO2 and water across
various loading levels in the ultra-microporous ZnAtzOx MOF. This
approach yields detailed information regarding the number of CO2 and water adsorption sites along with their locations, guest
dynamics, and host–guest interactions. Guest adsorption and
motional models proposed from NMR data are supported by computational
results, including visualizations of adsorption locations and the
spatial distribution of guests in different loading scenarios. The
wide variety and depth of information presented demonstrates how this
experimental methodology can be used to investigate humid carbon capture
and storage applications in other MOFs
Mechanochemical Synthesis of Methylammonium Lead Mixed–Halide Perovskites: Unraveling the Solid-Solution Behavior Using Solid-State NMR
Mixed-halide
lead perovskite (MHP) materials are rapidly advancing
as next-generation high-efficiency perovskite solar cells due to enhanced
stability and bandgap tunability. In this work, we demonstrate the
ability to readily and stoichiometrically tune the halide composition
in methylammonium-based MHPs using a mechanochemical synthesis approach.
Using this solvent-free protocol we are able to prepare domain-free
MHP solid solutions with randomly distributed halide ions about the
Pb center. Up to seven distinct [PbCl<sub><i>x</i></sub>Br<sub>6–x</sub>]<sup>4–</sup> environments are identified,
based on the <sup>207</sup>Pb NMR chemical shifts, which are also
sensitive to the changes in the unit cell dimensions resulting from
the substitution of Br by Cl, obeying Vegard’s law. We demonstrate
a straightforward and rapid synthetic approach to forming highly tunable
stoichiometric MHP solid solutions while avoiding the traditional
solution synthesis method by redirecting the thermodynamically driven
compositions. Moreover, we illustrate the importance of complementary
characterization methods, obtaining atomic-scale structural information
from multinuclear, multifield, and multidimensional solid-state magnetic
resonance spectroscopy, as well as from quantum chemical calculations
and long-range structural details using powder X-ray diffraction.
The solvent-free mechanochemical synthesis approach is also compared
to traditional solvent synthesis, revealing identical solid-solution
behavior; however, the mechanochemical approach offers superior control
over the stoichiometry of the final mixed-halide composition, which
is essential for device engineering