Magnetic behaviour and structure of polymeric oxovanadium carboxylates

1972 ◽  
Vol 25 (6) ◽  
pp. 1195 ◽  
Author(s):  
AT Casey ◽  
BSSE Morris ◽  
JR Thackeray

The synthesis and properties of a series of oxovanadium(1V) carboxylates (i.e. salts of organic acids) are described. The complexes closely resemble each other in magnetic properties, the observed paramagnetism being abnormally low for oxo-vanadium(1V) in the temperature range 90-350 K, with a broad maximum around 200-250 K. After testing of all reasonable models, the magnetic properties are interpreted in terms of anisotropic (Ising) antiferromagnetic exchange along infinite linear chains of interacting spins. On the basis of this model and with the aid of infrared, e.s.r., and electronic spectra, the most probable molecular structure for the series of complexes can be given. In our interpretation of the evidence, the interactions are of the super-exchange type.

1984 ◽  
Vol 62 (5) ◽  
pp. 891-898 ◽  
Author(s):  
John S. Haynes ◽  
Katherine W. Oliver ◽  
Steven J. Rettig ◽  
Robert C. Thompson ◽  
James Trotter

The preparation, magnetic and thermal properties, electronic and infrared spectra, and molecular structure of poly-bis(μ-di-n-hexylphosphinato)copper(II) are described. Crystals of the compound are triclinic, a = 9.800(3), b = 12.336(6), c = 13.352(8) Å, α = 88.53(3), β = 74.02(4), γ = 82.33(3)°, Z = 2, space group [Formula: see text]. The structure was solved by Patterson and Fourier syntheses and was refined by full-matrix least-squares procedures to R = 0.045 and Rw = 0.056 for 3095 reflections with I ≥ 3σ(I). The crystal structure of Cu[(n-C6H13)2PO2]2 consists of well-separated infinite chains of centro-symmetric spiro-fused eight-membered rings propagating along the crystallographic a axis.The magnetic susceptibility of Cu[(n-C6H13)2PO2]2 was studied over the temperature range 4.2 to 300 K. The compound shows ferromagnetic behaviour and the data have been successfully analyzed according to the isotropic Heisenberg model for linear chains with g = 2.16 and J = 2.58 cm−1. For comparison, the magnetic susceptibilities of Cu[(C2H5)2PO2]2 and Cu[(n-C4H9)2PO2]2 have also been measured over the range 4.2 to 300 K. The butyl derivative shows ferromagnetic exchange with g = 2.16 and J = 2.22 cm−1 while the ethyl derivative is antiferromagnetic with g = 2.19 and −J = 1.27 cm−1. The structural details of all three compounds are examined in the light of the differing magnetic properties.


Nanoscale ◽  
2021 ◽  
Author(s):  
Barbara Farkas ◽  
Nora Henriette De Leeuw

Implementation of magnetic nanoparticles in biomedicine requires their passivation, which often comes at a cost of diminished magnetic properties. For the design of nano-agents with targeted magnetic behaviour, it is...


2012 ◽  
Vol 41 (6) ◽  
pp. 620-621 ◽  
Author(s):  
Young Hoon Lee ◽  
Kazuya Kato ◽  
Emi Kubota ◽  
Satoshi Kawata ◽  
Shinya Hayami

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