2016
DOI: 10.1016/j.jmmm.2015.10.024
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The superexchange interactions and magnetic ordering in low-dimentional ludwigite Ni 5 GeB 2 O 10

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Cited by 17 publications
(19 citation statements)
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“…One can observe an anomalous behavior with a temperature peak at T c =88.1 K. The lattice specific heat was determined using linear combinations of the Debye-Einstein functions with the characteristic temperatures found to be T D = 331 K and T E = 780 K. It can be seen that the low temperature region isnot correctly interpolated. The same behavior was previously observed in another ludwigite crystal, Ni 5 GeB 2 O 10 [13]. Subtracting the lattice contribution to the specific heat from the experimental data, we found the excess specific heat and the phase transition entropy ∆S= 0.6 J/(mol*K).…”
Section: 3supporting
confidence: 87%
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“…One can observe an anomalous behavior with a temperature peak at T c =88.1 K. The lattice specific heat was determined using linear combinations of the Debye-Einstein functions with the characteristic temperatures found to be T D = 331 K and T E = 780 K. It can be seen that the low temperature region isnot correctly interpolated. The same behavior was previously observed in another ludwigite crystal, Ni 5 GeB 2 O 10 [13]. Subtracting the lattice contribution to the specific heat from the experimental data, we found the excess specific heat and the phase transition entropy ∆S= 0.6 J/(mol*K).…”
Section: 3supporting
confidence: 87%
“…Although the compound under study is dielectric, at temperatures close to zero, the specific heat decreases in accordance with the linear law, which were observed for all investigated ludwigites [13,22].…”
Section: Thermodynamic Propertiessupporting
confidence: 65%
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“…The field dependence of the magnetization has a “plateau” or “jumps” when the field is along the b axis. Similar behavior has been observed in some cobalt ludwigites: Co 5 TiBO 5 , CoMgGaBO 5 , the authors has attributed this behavior to the spin‐glass magnetic order, but Co 5 Sn(BO 5 ) 2 , in which such hysteresis loops behavior is observed, enters the magnetically ordered state at 82 K. In the case of nickel‐germanium ludwigite, such behavior is observed in a field in the only one direction, and possibly due to the partial reorientation of the sublattices .…”
Section: Heterometallic Ludwigitessupporting
confidence: 74%
“…The ludwigites Ni 5 Ge(BO 5 ) 2 , Ni 5 Zr(BO 5 ) 2 , and Ni 5 Ti(BO 5 ) 2 have a disordered distribution of nonmagnetic ions, with smaller (for Ge) or larger (for Ti and Zr) radii than the Sn ion. An interesting question is how the ordered distribution of Sn influences the magnetic properties of Ni 5 Sn(BO 5 ) 2 , and whether the unusual properties of Ni 5 Ge(BO 5 ) 2 arise . In a previous study, we reported the very interesting magnetic properties of Ni 5 Ge(BO 5 ) 2 .…”
Section: Introductionmentioning
confidence: 99%