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Close Encounters of the Weak Kind: Investigations of Electron–Electron Interactions between Dissimilar Spins in Hybrid Rotaxanes
[Image: see text] We report a family of hybrid [2]rotaxanes based on inorganic [Cr(7)NiF(8)(O(2)C(t)Bu)(16)](−) (“{Cr(7)Ni}”) rings templated about organic threads that are terminated at one end with pyridyl groups. These rotaxanes can be coordinated to [Cu(hfac)(2)] (where Hhfac = 1,1,1,5,5,5-hexaf...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2019
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6814243/ https://www.ncbi.nlm.nih.gov/pubmed/31411874 http://dx.doi.org/10.1021/jacs.9b05590 |
Sumario: | [Image: see text] We report a family of hybrid [2]rotaxanes based on inorganic [Cr(7)NiF(8)(O(2)C(t)Bu)(16)](−) (“{Cr(7)Ni}”) rings templated about organic threads that are terminated at one end with pyridyl groups. These rotaxanes can be coordinated to [Cu(hfac)(2)] (where Hhfac = 1,1,1,5,5,5-hexafluoroacetylacetone), to give 1:1 or 1:2 Cu:{Cr(7)Ni} adducts: {[Cu(hfac)(2)](py-CH(2)NH(2)CH(2)CH(2)Ph)[Cr(7)NiF(8)(O(2)C(t)Bu)(16)]}, {[Cu(hfac)(2)][py-CH(2)NH(2)CH(2)CH(3)][Cr(7)NiF(8)(O(2)C(t)Bu)(16)]}, {[Cu(hfac)(2)]([py-CH(2)CH(2)NH(2)CH(2)C(6)H(4)SCH(3)][Cr(7)NiF(8)(O(2)C(t)Bu)(16)])(2)}, {[Cu(hfac)(2)]([py-C(6)H(4)-CH(2)NH(2)(CH(2))(4)Ph][Cr(7)NiF(8)(O(2)C(t)Bu)(16)])(2)}, and {[Cu(hfac)(2)]([3-py-CH(2)CH(2)NH(2)(CH(2))(3)SCH(3)][Cr(7)NiF(8)(O(2)C(t)Bu)(16)])(2)}, the structures of which have been determined by X-ray diffraction. The {Cr(7)Ni} rings and Cu(II) ions both have electronic spin S = 1/2, but with very different g-values. Continuous-wave EPR spectroscopy reveals the exchange interactions between these dissimilar spins, and hence the communication between the different molecular components that comprise these supramolecular systems. The interactions are weak such that we observe AX or AX(2) type spectra. The connectivity between the {Cr(7)Ni} ring and thread terminus is varied such that the magnitude of the exchange interaction J can be tuned. The coupling is shown to be dominated by through-bond rather than through-space mechanisms. |
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