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dc.contributor.authorBiswas, S-
dc.contributor.authorBejoymohandas, K S-
dc.contributor.authorDas, S-
dc.contributor.authorKalita, P-
dc.contributor.authorReddy, M L P-
dc.contributor.authorOyarzabal, I-
dc.contributor.authorColacio, E-
dc.contributor.authorChandrasekhar, V-
dc.date.accessioned2017-10-13T10:53:08Z-
dc.date.available2017-10-13T10:53:08Z-
dc.date.issued2017-06-29-
dc.identifier.citationInorganic Chemistry,56(14):7985–7997en_US
dc.identifier.urihttp://hdl.handle.net/123456789/2946-
dc.description.abstractThe sequential reaction of 2-((6-(hydroxymethyl)pyridin-2-yl)-methyleneamino)phenol (LH2), LnCl3·6H2O, and 1,1,1-trifluoroacetylacetone (Htfa) in the presence of Et3N afforded [Ln(LH) (tfa)2] [Ln = Dy3+ (1), Ln = Tb3+ (2), and Ln = Gd3+ (3)], while under the same reaction conditions, but in the absence of the coligand, another series of mononuclear complexes, namely, [Ln(LH)2]·Cl·2MeOH] [Ln = Dy3+ (4) and Tb3+ (5)] are obtained. Singlecrystal X-ray diffraction analysis revealed that the former set contains a mono-deprotonated [LH]− and two tfa ligands, while the latter set comprises of two mono-deprotonated [LH]− ligands that are nearly perpendicular to each other at an angle of 86.9°. Among these complexes, 2 exhibited a ligand-sensitized lanthanide-characteristic emission. Analyses of the alternating current susceptibility measurements reveal the presence of single-molecule magnet behavior for 1 and 4, in the presence of direct-current field, with effective energy barriers of 4.6 and 44.4 K, respectively. The enhancement of the effective energy barrier of the latter can be attributed to the presence of a large energy gap between the ground and first excited Kramers doublets, triggered by the change in coordination environments around the lanthanide centers.en_US
dc.language.isoenen_US
dc.publisherAmerican Chemical Societyen_US
dc.titleMononuclear Lanthanide Complexes: Energy-Barrier Enhancement by Ligand Substitution in Field-Induced DyIII SIMsen_US
dc.typeArticleen_US
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