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. 2020 Sep 8;59(17):12758-12767.
doi: 10.1021/acs.inorgchem.0c01816. Epub 2020 Aug 27.

Paramagnetic Shifts and Guest Exchange Kinetics in ConFe4- n Metal-Organic Capsules

Affiliations

Paramagnetic Shifts and Guest Exchange Kinetics in ConFe4- n Metal-Organic Capsules

Kang Du et al. Inorg Chem. .

Abstract

We investigate the magnetic resonance properties and exchange kinetics of guest molecules in a series of hetero-bimetallic capsules, [ConFe4-nL6]4- (n = 1-3), where L2- = 4,4'-bis[(2-pyridinylmethylene)amino]-[1,1'-biphenyl]-2,2'-disulfonate. H bond networks between capsule sulfonates and guanidinium cations promote the crystallization of [ConFe4-nL6]4-. The following four isostructural crystals are reported: two guest-free forms, (C(NH2)3)4[Co1.8Fe2.2L6]·69H2O (1) and (C(NH2)3)4[Co2.7Fe1.3L6]·73H2O (2), and two Xe- and CFCl3-encapsulated forms, (C(NH2)3)4[(Xe)0.8Co1.8Fe2.2L6]·69H2O (3) and (C(NH2)3)4[(CFCl3)Co2.0Fe2.0L6]·73H2O (4), respectively. Structural analyses reveal that Xe induces negligible structural changes in 3, while the angles between neighboring phenyl groups expand by ca. 3° to accommodate the much larger guest, CFCl3, in 4. These guest-encapsulated [ConFe4-nL6]4- molecules reveal 129Xe and 19F chemical shift changes of ca. -22 and -10 ppm at 298 K, respectively, per substitution of low-spin FeII by high-spin CoII. Likewise, the temperature dependence of the 129Xe and 19F NMR resonances increases by 0.1 and 0.06 ppm/K, respectively, with each additional paramagnetic CoII center. The optimal temperature for hyperpolarized (hp) 129Xe chemical exchange saturation transfer (hyper-CEST) with [ConFe4-nL6]4- capsules was found to be inversely proportional to the number of CoII centers, n, which is consistent with the Xe chemical exchange accelerating as the portals expand. The systematic study was facilitated by the tunability of the [M4L6]4- capsules, further highlighting these metal-organic systems for developing responsive sensors with highly shifted 129Xe resonances.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Figure 1.
Figure 1.
Preparation schemes and structures for 1 and 2 (a), 3 (b), and 4 (c). Disordered H2O molecules and H atoms are omitted for clarity. Green, purple, yellow, cyan, red, blue, and gray spheres represent Co/Fe, Cl, S, F, O, N, and C atoms, respectively.
Figure 2.
Figure 2.
Variable-temperature 19F NMR spectra for an aqueous sample containing 5 mM 4. Legend indicates the experimental temperature in the unit of K. Dotted boxes indicate the 19F peak assignments for [(CFCl3)MII4L6]4– molecules and * suggests the position for free CFCl3, which is used as reference.
Figure 3.
Figure 3.
Stacked 129Xe NMR spectra for aqueous samples containing 200 μM 1 (black and red), 2 (blue), and 100 μM 5 (orange) collected at 278 K, with Eburp1-shaped pulses (660 Hz width) applied at –22.6, –49.7, –72.8, and –94.4 ppm, respectively.
Figure 4.
Figure 4.
Z-spectra of an aqueous solution containing 10 μM 1 collected at 298 K with 2.3 s presaturation pulses applied at 5 ppm intervals with an averaged B1 = 30 μT. Highlighted regions in pink, gray, red, blue, and orange indicated the resonances at +15, –20, –45, –70, and –90 ppm.
Figure 5.
Figure 5.
Top: Variable-temperature z-spectra for an aqueous sample containing 10 μM 1 collected with 2.3 s presaturation pulses applied at 2 ppm intervals with an averaged saturation power B1 = 12 μT. The legend indicates the experimental temperatures in the unit of K. Circles and solid lines represent experimental data and Lorentzian fits, respectively, except for 278 K, where the purple solid line represents connection of experimental data points. Bottom: Temperature-dependent 129Xe chemical shifts for [(Xe)CoFe3L6]4– (black), [(Xe)Co2Fe2L6]4– (red), and [(Xe)Co3FeL6]4– (blue), which are summarized from variable-temperature CEST experiments. The chemical shifts are referenced to 129Xe(aq) signal.

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