Alternating spin chains: Controlled assembly from bimetallic building blocks and QMC simulation of spin correlation

2007 | journal article. A publication with affiliation to the University of Göttingen.

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​Alternating spin chains: Controlled assembly from bimetallic building blocks and QMC simulation of spin correlation​
Demeshko, S.; Leibeling, G.; Dechert, S. ; Fuchs, S.; Pruschke, T. & Meyer, F.​ (2007) 
ChemPhysChem8(3) pp. 405​-417​.​ DOI: https://doi.org/10.1002/cphc.200600586 

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Authors
Demeshko, Serhiy; Leibeling, Guido; Dechert, Sebastian ; Fuchs, Sebastian; Pruschke, Thomas; Meyer, Franc
Abstract
By using the compartmental dinucleating pyrazolate ligand HL, dinickel(ll) complexes [LNi2(mu-N-3)(acetone)(2)]X-2, (1: X=ClO4; 2: X=BPh4) and tetranickel(ll) complex [{LNi2(mu-N-3)(MeOH)}(2)](ClO4)(4) (3) have been prepared and structurally characterized. Complexes I and 2 differ in the torsion along the bridging mu-1,3-azide moiety, while the azido ligands in 3 adopt an unusual mu-1, 1,3 bridging mode to connect the two subunits. All three complexes show overall antiferromagnetic coupling and on S=0 ground state, but the torsion along the azide moiety is a determining factor for the coupling strength. Compounds I and 2 serve as preorganized building blocks for the controlled synthesis of alternating ID polymeric structures 4-6 by replacement of their labile acetone ligands by additional azido ligands. Due to the modular synthetic approach, 4-6 can be described as Heisenberg antiferromagnetic systems with inherent bond alternation (HABA), whereby the organic ligand framework ensures that the individual nickel/azido chains are well isolated in the crystal lattice. Like their precursors, 4-6 are mainly distinguished by torsion along the mu-1,3-azido bridges, both within and between the bimetallic constituents. Magnetic measurements confirm on overall S=0 ground state for 4-6, and coupling parameters hove been deduced from quantum Monte Carlo simulations. The two J values for the alternating 1D chains can be clearly assigned on the basis of the magnetostructural correlations established for the bimetallic building blocks. The alternation ratio gamma=J(2)J(1)(-1) places the three new systems in the HABA regime for a singlet-dimer ground state.
Issue Date
2007
Status
published
Publisher
Wiley-v C H Verlag Gmbh
Journal
ChemPhysChem 
ISSN
1439-7641; 1439-4235

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