2005
DOI: 10.1039/b509810f
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A Cu–Zn–Cu–Zn heterometallomacrocycle shows significant antiferromagnetic coupling between paramagnetic centres mediated by diamagnetic metal

Abstract: An unprecedented antiferromagnetic exchange mediated by two -O-Zn-O- bridges, with singlet-triplet splitting J= 35.0 cm-1, was observed between two copper centers separated by 5.7062(9)A in the heterometallomacrocyclic diethanolamine (H2L) complex [Cu2Zn2(NH3)2Br2(HL)4]Br2.CH3OH.

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Cited by 60 publications
(51 citation statements)
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“…The obtained values ⊥ > g g || point out that the unpaired electron is located in the 2 2 y x d − orbital, in accord with the squarepyramidal environment around the copper(II) centres [42]. With a rise of temperature, the number of binuclear copper(II) units of compound 1, that were excited from the ground spinsinglet state (S = 0) to the higher spin-triplet state (S = 1) grew up [39]. The spins S = 1 became magnetically diluted centres in the mainly diamagnetic lattice (S = 0).…”
Section: Epr Studymentioning
confidence: 51%
See 1 more Smart Citation
“…The obtained values ⊥ > g g || point out that the unpaired electron is located in the 2 2 y x d − orbital, in accord with the squarepyramidal environment around the copper(II) centres [42]. With a rise of temperature, the number of binuclear copper(II) units of compound 1, that were excited from the ground spinsinglet state (S = 0) to the higher spin-triplet state (S = 1) grew up [39]. The spins S = 1 became magnetically diluted centres in the mainly diamagnetic lattice (S = 0).…”
Section: Epr Studymentioning
confidence: 51%
“…Fitting the Curie dependence to the experimental data reveals that 5.9% of the copper(II) ions in the sample of 1 are not coupled into dimers. The presence of the non-coupled copper(II) impurities(evidenced at the lowest temperatures through a slight increase in χ ) is a phenomenon common for this type of antiferromagnetic species[39].The coupling of two copper(II) ions through the oxalate-bridge makes a strong exchange interaction, with J = -295(2) and-294(2) cm -1 for 1 and 2, respectively. It is known that in the complexes with two square-pyramidal copper(II) centres and an entirely planar [LCu(magnetic orbital of copper(II) should be ideally directed towards the oxalate σ orbitals, and the antiferromagnetic interaction would be maximized (J from -280 to -400 cm -1 )[32a].…”
mentioning
confidence: 99%
“…0.027 cm 3 K mol −1 at 2 K. On the other hand, the χ m vs T curve provides more information about the magnetic behavior of complex 1: the χ m value of 0.034 cm −3 mol at room temperature increases as the temperature decreases, arriving at a maximum value of 0.082 cm −3 mol at 45 K; χ m then decreases practically to 0.012 cm −3 mol at 3 K before increasing a value of 0.013 cm −3 mol at 2 K. This behavior clearly indicates a typical antiferromagnetic coupling and the presence of a small amount of paramagnetic impurities. 17 The reciprocal molar magnetic susceptibility data obey the Curie−Weiss law in the high temperature region of 50−300 K with a Curie constant of C = 14.46 cm 3 K mol −1 and a Weiss constant of θ = −113.92 K. The negative value of the Weiss temperature, together with the curve of χ m T (T), indicates the presence of strong antiferromagnetic coupling between nickel(II) ions.…”
Section: ■ Results and Discussionmentioning
confidence: 98%
“…The cyclic motif 2M4‐1 is an evolution (Table 1) of the consecutive motif 1,2M4‐1 described above and exemplified by complexes 6 – 9 . The heterometallic Cu/Zn coordination compound 10 ,20 the structure of which belongs to the cyclic motif 2M4‐1 , was obtained by reaction (17).…”
Section: Complexes Of Tetranuclear Structuresmentioning
confidence: 99%