Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5205
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)
Authors: Ahmed, Naushad
Das, Chinmoy
Vaidya, Shefali
SRIVASTAVA, ANANT KUMAR
Langley, Stuart K.
Murray, Keith S.
Shanmugam, Maheswaran
Dept. of Chemistry
Keywords: Single-Molecule-Magnet
Palladium-Catalyzed Synthesis
Biomedical Applications
Dilanthanide Complexes
M-II-LN(III)-M-II M
Crystal-Structures
Slow Relaxation
DY Complexes
Metal-Ions
Clusters
2014
Issue Date: Dec-2014
Publisher: Royal Society of Chemistry
Citation: Dalton Transactions, 43(46),17375-17384.
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.
URI: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5205
https://doi.org/10.1039/C4DT02360A
ISSN: 1477-9226
1477-9234
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