2005
DOI: 10.1002/pssb.200562463
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Magnetic properties of TM3[Cr(CN)6]2·n H2O

Abstract: Magnetization measurements performed on Prussian blue analogs Mn, Fe, Co, Ni, Cu) confirmed the dual character of the exchange interaction (antiferromagnetic AFM and ferromagnetic FM) in this system. AFM interaction dominates for the Cr 2+ sample and with rising atomic number Z the FM interaction becomes more important reaching pure FM character for the Cu 2+ sample.

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Cited by 10 publications
(14 citation statements)
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“…3 (e g ) 1 leading to 3 F and 9 AF pathways, or the second possibility when Cr 2+ is low spin S = 1 and magnetic orbitals are (t 2g ) 2 leading to 6 AF pathways [4]. In the case that all Cr 2+ are high spin, the expected theoretical value …”
Section: Resultsmentioning
confidence: 95%
See 1 more Smart Citation
“…3 (e g ) 1 leading to 3 F and 9 AF pathways, or the second possibility when Cr 2+ is low spin S = 1 and magnetic orbitals are (t 2g ) 2 leading to 6 AF pathways [4]. In the case that all Cr 2+ are high spin, the expected theoretical value …”
Section: Resultsmentioning
confidence: 95%
“…3 (e g ) 1 and low spin S = 1 with magnetic orbitals (t 2g ) 2 as well [4]. In our recent paper [5] we presented results of the pressure effect on magnetic properties of TM …”
Section: Introductionmentioning
confidence: 92%
“…The magnetic coupling in these systems is determined by super-exchange interaction between metal ions A 2+ and B III mediated through a three-dimensional network of C¨CN bridges, resulting in 3D magnetic ordering with transition temperatures T C up to 376 K [2] depending on the nature of the metal ions. The magnetic properties of PBA can be analysed within two simplifications: (i) only the superexchange interactions between the nearest neighbour metal A 2+ and B III ions have to be considered; (ii) if the magnetic orbital symmetries of the metal ions are the same, the super-exchange interaction is antiferromagnetic (J AF ); conversely, when their magnetic orbital symmetries are different, the super-exchange interaction is ferromagnetic (J F 3 (e g ) 2 orbitals of Mn 2+ leading to overall J AF interaction. The large number of possible combinations of ions and oxidation states give rise to many competing orbital interactions, which will cause the structure to reach an overall order, either fero or ferimagnetic.…”
Section: Introductionmentioning
confidence: 99%
“…Later in paper [5] −N ≡ C−B III ) ions have to be considered; (ii) if the magnetic orbital symmetries of the metal ions are the same, the superexchange interaction is antiferromagnetic (J AF ); conversely, when their magnetic orbital symmetries are different, the super-exchange interaction is ferromagnetic (J F ). The cluster glass behaviour is frequently observed in this system [6,7]. The results of the pressure effect on magnetic properties of the mother PBA were recently published in [8].…”
Section: Introductionmentioning
confidence: 88%