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Probing the magnetic and magnetothermal properties of M(ii)–Ln(iii) complexes (where M(ii) = Ni or Zn; Ln(iii) = La or Pr or Gd)

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dc.contributor.author Ahmed, Naushad en_US
dc.contributor.author Das, Chinmoy en_US
dc.contributor.author Vaidya, Shefali en_US
dc.contributor.author SRIVASTAVA, ANANT KUMAR en_US
dc.contributor.author Langley, Stuart K. en_US
dc.contributor.author Murray, Keith S. en_US
dc.contributor.author Shanmugam, Maheswaran en_US
dc.date.accessioned 2020-10-20T07:06:50Z
dc.date.available 2020-10-20T07:06:50Z
dc.date.issued 2014-12 en_US
dc.identifier.citation Dalton Transactions, 43(46),17375-17384. en_US
dc.identifier.issn 1477-9226 en_US
dc.identifier.issn 1477-9234 en_US
dc.identifier.uri http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5205
dc.identifier.uri https://doi.org/10.1039/C4DT02360A en_US
dc.description.abstract We 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.iso en en_US
dc.publisher Royal Society of Chemistry en_US
dc.subject Single-Molecule-Magnet en_US
dc.subject Palladium-Catalyzed Synthesis en_US
dc.subject Biomedical Applications en_US
dc.subject Dilanthanide Complexes en_US
dc.subject M-II-LN(III)-M-II M en_US
dc.subject Crystal-Structures en_US
dc.subject Slow Relaxation en_US
dc.subject DY Complexes en_US
dc.subject Metal-Ions en_US
dc.subject Clusters en_US
dc.subject 2014 en_US
dc.title Probing 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.type Article en_US
dc.contributor.department Dept. of Chemistry en_US
dc.identifier.sourcetitle Dalton Transactions en_US
dc.publication.originofpublisher Foreign en_US


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