The surface of γ-alumina nanoparticles can be characterized by dynamic nuclear polarization (DNP) surface-enhanced NMR of (27)Al. DNP is combined with cross-polarization and MQ-MAS to determine local symmetries of (27)Al sites at the surface.
We show that dynamic nuclear polarization (DNP) can be used to enhance NMR signals of13C and 29Si nuclei located in mesoporous organic/inorganic hybrid materials, at several hundreds of nanometers from stable radicals (TOTAPOL) trapped in the surrounding frozen disordered water. The approach is demonstrated using mesoporous silica nanoparticles (MSN), functionalized with 3-(N-phenylureido)propyl (PUP) groups, filled with the surfactant cetyltrimethylammonium bromide (CTAB). The DNP-enhanced proton magnetization is transported into the mesopores via 1H-1H spin diffusion and transferred to rare spins by cross-polarization, yielding signal enhancements εon/off of around 8. When the CTAB molecules are extracted, so that the radicals can enter the mesopores, the enhancements increase to εon/off ≈ 30 for both nuclei. A quantitative analysis of the signal enhancements in MSN with and without surfactant is based on a one-dimensional proton spin diffusion model. The effect of solvent deuteration is also investigated.
Disciplines
Chemistry
CommentsReprinted (adapted) with permission from Journal of Physical Chemistry C 117 (2013) ABSTRACT: We show that dynamic nuclear polarization (DNP) can be used to enhance NMR signals of 13 C and 29 Si nuclei located in mesoporous organic/ inorganic hybrid materials, at several hundreds of nanometers from stable radicals (TOTAPOL) trapped in the surrounding frozen disordered water. The approach is demonstrated using mesoporous silica nanoparticles (MSN), functionalized with 3-(N-phenylureido)propyl (PUP) groups, filled with the surfactant cetyltrimethylammonium bromide (CTAB). The DNP-enhanced proton magnetization is transported into the mesopores via 1 H− 1 H spin diffusion and transferred to rare spins by cross-polarization, yielding signal enhancements ε on/off of around 8. When the CTAB molecules are extracted, so that the radicals can enter the mesopores, the enhancements increase to ε on/off ≈ 30 for both nuclei. A quantitative analysis of the signal enhancements in MSN with and without surfactant is based on a one-dimensional proton spin diffusion model. The effect of solvent deuteration is also investigated.
Fibrous nanosilica (KCC-1) oxynitrides are promising solid-base catalysts. Paradoxically, when their nitrogen content increases, their catalytic activity decreases. This counterintuitive observation is explained here for the first time using 15 N-solid-state NMR spectroscopy enhanced by dynamic nuclear polarization.
N Broadband excitation DANTE MAS Paramagnetic samples a b s t r a c tWe analyze the direct excitation of wide one-dimensional spectra of nuclei with spin I = 1/2 or 1 in rotating solids submitted to pulse trains in the manner of Delays Alternating with Nutations for Tailored Excitation (DANTE), either with one short rotor-synchronized pulse of duration s p in each of K rotor periods For nuclei with I = 1 (e.g., for 14 N), the response to basic D K 1 pulse train is moreover affected by inhomogeneous decay due to 2nd-order quadrupole interactions, since these are not of rank 2 and therefore cannot be eliminated by spinning about the magic angle. For large quadrupole interactions, the signal decay produced by second-order quadrupole interaction can be minimized by (i) reducing the length of D K N pulse trains using N > 1, (ii) fast spinning, (iii) large rf-field, and (iv) using high magnetic fields to reduce the 2nd-order quadrupole interaction.
The local structure and cation disorder in Y2(Sn,Ti)2O7 pyrochlores, materials proposed
for the encapsulation
of lanthanide- and actinide-bearing radioactive waste, is investigated
using 89Y (I = 1/2) NMR spectroscopy and,
in particular, measurement of the 89Y anisotropic shielding.
Although known to be a good probe of the local environment, information
on the anisotropy of the shielding interaction is removed under magic
angle spinning (MAS). Here, we consider the feasibility of experimental
measurement of the 89Y anisotropic shielding interaction
using two-dimensional CSA-amplified PASS experiments, implemented
for 89Y for the first time. Despite the challenges associated
with the study of low-γ nuclei, and those resulting from long
T1 relaxation times, the successful implementation of these
experiments is demonstrated for the end member pyrochlores, Y2Sn2O7 and Y2Ti2O7. The accuracy and robustness of the measurement to
various experimental parameters is also considered, before the approach
is then applied to the disordered materials in the solid solution.
The anisotropies extracted for each of the sideband manifolds are
compared to those obtained using periodic first-principles calculations,
and provide strong support for the assignment of the spectral resonances.
The value of the span, Ω, is shown to be a sensitive probe of
the next nearest neighbor (NNN) environment, i.e., the number of Sn
and Ti on the six surrounding “B” (i.e., six-coordinate)
sites, and also provides information on the local geometry directly,
through a correlation with the average Y–O8b distance
(where 8b indicates the
Wyckoff position of the oxygen).
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