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dc.contributor.authorAhmed, Naushaden_US
dc.contributor.authorDas, Chinmoyen_US
dc.contributor.authorVaidya, Shefalien_US
dc.contributor.authorSRIVASTAVA, ANANT KUMARen_US
dc.contributor.authorLangley, Stuart K.en_US
dc.contributor.authorMurray, Keith S.en_US
dc.contributor.authorShanmugam, Maheswaranen_US
dc.date.accessioned2020-10-20T07:06:50Z-
dc.date.available2020-10-20T07:06:50Z-
dc.date.issued2014-12en_US
dc.identifier.citationDalton Transactions, 43(46),17375-17384.en_US
dc.identifier.issn1477-9226en_US
dc.identifier.issn1477-9234en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5205-
dc.identifier.urihttps://doi.org/10.1039/C4DT02360Aen_US
dc.description.abstractWe establish the coordination potential of the Schiff base ligand (2-methoxy-6-[(E)-2′-hydroxymethyl-phenyliminomethyl]-phenolate (H2L)) via the isolation of various M(II)–Ln(III) complexes (where M(II) = Ni or Zn and Ln(III) = La or Pr or Gd). Single crystals of these five complexes were isolated and their solid state structures were determined by single crystal X-ray diffraction. Structural determination revealed molecular formulae of [NiGd(HL)2(NO3)3] (1), [NiPr(HL)2(NO3)3] (2) and [Ni2La(HL)4(NO3)](NO3)2 (3), [Zn2Gd(HL)4(NO3)](NO3)2 (4), and [Zn2Pr(HL)4(NO3)](NO3)2 (5). Complexes 1 and 2 were found to be neutral heterometallic dinuclear compounds, whereas 3–5 were found to be linear heterometallic trinuclear cationic complexes. Direct current (dc) magnetic susceptibility and magnetization measurements conclusively revealed that complexes 1 and 4 possess a spin ground state of S = 9/2 and 7/2 respectively. Empirically calculated ΔχMT derived from the variable temperature susceptibility data for all complexes undoubtedly indicates that the Ni(II) ion is coupled ferromagnetically with the Gd(III) ion, and antiferromagnetically with the Pr(III) ion in 1 and 2 respectively. The extent of the exchange interaction for 1 was estimated by fitting the magnetic susceptibility data using the parameters (g = 2.028, S = 9/2, J = 1.31 cm−1 and zJ = +0.007), supporting the phenomenon observed in an empirical approach. Similarly using a HDVV Hamiltonian, the magnetic data of 3 and 4 were fitted, yielding parameters g = 2.177, D = 3.133 cm−1, J = −0.978 cm−1, (for 3) and g = 1.985, D = 0.508 cm−1 (for 4). The maximum change in magnetic entropy (−ΔSm) estimated from the isothermal magnetization data for 1 was found to be 5.7 J kg−1 K−1 (ΔB = 7 Tesla) at 7.0 K, which is larger than the −ΔSm value extracted from 4 of 3.5 J kg−1 K−1 (ΔB = 7 Tesla) at 15.8 K, revealing the importance of the exchange interaction in increasing the overall ground state of a molecule for better MCE efficiency.en_US
dc.language.isoenen_US
dc.publisherRoyal Society of Chemistryen_US
dc.subjectSingle-Molecule-Magneten_US
dc.subjectPalladium-Catalyzed Synthesisen_US
dc.subjectBiomedical Applicationsen_US
dc.subjectDilanthanide Complexesen_US
dc.subjectM-II-LN(III)-M-II Men_US
dc.subjectCrystal-Structuresen_US
dc.subjectSlow Relaxationen_US
dc.subjectDY Complexesen_US
dc.subjectMetal-Ionsen_US
dc.subjectClustersen_US
dc.subject2014en_US
dc.titleProbing the magnetic and magnetothermal properties of M(ii)–Ln(iii) complexes (where M(ii) = Ni or Zn; Ln(iii) = La or Pr or Gd)en_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Chemistryen_US
dc.identifier.sourcetitleDalton Transactionsen_US
dc.publication.originofpublisherForeignen_US
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