1971
DOI: 10.1071/ch9710441
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The nuclear magnetic resonance spectra of 4,4'-Dimethyl-2,2'-bipyridyl complexes of iron, ruthenium, and osmium

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Cited by 21 publications
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“…The 1 H NMR spectral data of cis -[Ru(bpy) 2 (NH 3 ) 2 ] 2+ are given in the Experimental Section, and the peaks are assigned according to the following diagram: When compared to the free uncoordinated ligand, the H6 proton of the cis -[Ru(bpy) 2 (NH 3 ) 2 ] 2+ complex shows a significant downfield shift (8.7 and 9.1 ppm, respectively), which is consistent with a cis arrangement where the π-cloud of the adjacent ligand induces a diamagnetic anisotropic effect. The 1 H NMR data clearly indicate that the pyridines within each bpy ligand in cis -[Ru(bpy) 2 (NH 3 ) 2 ] 2+ are magnetically nonequivalent. As a result, out of the possible 8-proton resonance peaks, seven distinct bands were observed in DMSO solvent with the peaks for the H5 and H4‘ protons overlaping.
…”
Section: Resultsmentioning
confidence: 98%
See 1 more Smart Citation
“…The 1 H NMR spectral data of cis -[Ru(bpy) 2 (NH 3 ) 2 ] 2+ are given in the Experimental Section, and the peaks are assigned according to the following diagram: When compared to the free uncoordinated ligand, the H6 proton of the cis -[Ru(bpy) 2 (NH 3 ) 2 ] 2+ complex shows a significant downfield shift (8.7 and 9.1 ppm, respectively), which is consistent with a cis arrangement where the π-cloud of the adjacent ligand induces a diamagnetic anisotropic effect. The 1 H NMR data clearly indicate that the pyridines within each bpy ligand in cis -[Ru(bpy) 2 (NH 3 ) 2 ] 2+ are magnetically nonequivalent. As a result, out of the possible 8-proton resonance peaks, seven distinct bands were observed in DMSO solvent with the peaks for the H5 and H4‘ protons overlaping.
…”
Section: Resultsmentioning
confidence: 98%
“…The 1 H NMR data clearly indicate that the pyridines within each bpy ligand in cis-[Ru(bpy) 2 (NH 3 ) 2 ] 2+ are magnetically nonequivalent. [30][31][32] As a result, out of the possible 8-proton resonance peaks, seven distinct bands were observed in DMSO solvent with the peaks for the H5 and H4′ protons overlaping.…”
Section: Resultsmentioning
confidence: 99%
“…The same arguments apply to the other two terms which appear in eq 19, and so to lowest nonvanishing order we may write the contribution to the dipole strength which arises from static-vibrational interactions as Z)VS(A->-J) = DrVS(A-»J) (21) Note that the additivity properties with respect to the vibrational perturbations are preserved in eq 21. Since the magneto-optical B term has the same symmetry properties as the dipole strength, we may write ß( ->J) as S(A^J) = SV(A^J) + BS(A^J) + fivs(A-*J) + higher-order terms = *,V(A-J) + Srs(A-J) r + 5rVS(A-*-J) + higher-order terms (22) Here Bf is the purely vibrational contribution of the nontotally symmetric normal mode Qr to the B term associated with the | A) -| J) transition, 5rs is the purely static contribution of £/(T), and Brws is the contribution of static-vibrational interactions. Brws is of second order in the normal coordinate Qr and first order in the totally symmetric component of the static perturbation.…”
Section: If the | A0) -*mentioning
confidence: 97%
“…Crystal data: space group, PI; a = 9.272 (2) Á, b = 13.727 (2) A,c = 8.973 (1) A, a = 103. 44 (1)°, ß = 120. 53 (1)°, y = 90.01 (1)°, K = 947.1 (3) A3, Z = 2.…”
mentioning
confidence: 99%