5 research outputs found

    Strong Magnetocaloric Coupling in Oxyorthosilicate with Dense Gd<sup>3+</sup> Spins

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    Searching for working refrigerant materials is the key element in the design of magnetic cooling devices. Herein, we report on the thermodynamic and magnetocaloric parameters of an X1 phase oxyorthosilicate, Gd2SiO5, by field-dependent static magnetization and specific heat measurements. An overall correlation strength of |J|S2 ā‰ˆ 3.4 K is derived via the mean-field estimate, with antiferromagnetic correlations between the ferromagnetically coupled Gdā€“Gd layers. The magnetic entropy change āˆ’Ī”Sm is quite impressive, reaches 0.40 J Kā€“1 cmā€“3 (58.5 J Kā€“1 kgā€“1) at T = 2.7 K, with the largest adiabatic temperature change Tad = 23.2 K for a field change of 8.9 T. At T = 20 K, the lattice entropy SL is small enough compared to the magnetic entropy Sm, Sm/SL = 21.3, which warrants its potential in 2 āˆ’20 K cryocoolers with both the Stirling and Carnot cycles. Though with relatively large exchange interactions, the layered A-type spin arrangement ultimately enhances the magnetocaloric coupling, raising the possibilities of designing magnetic refrigerants with a high ratio of cooling capacity to volume

    LaMn<sub>3</sub>Ni<sub>2</sub>Mn<sub>2</sub>O<sub>12</sub>: An A- and Bā€‘Site Ordered Quadruple Perovskite with Aā€‘Site Tuning Orthogonal Spin Ordering

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    A new oxide, LaMn<sub>3</sub>Ni<sub>2</sub>Mn<sub>2</sub>O<sub>12</sub>, was prepared by high-pressure and high-temperature synthesis methods. The compound crystallizes in an AAā€²<sub>3</sub>B<sub>2</sub>Bā€²<sub>2</sub>O<sub>12</sub>-type A-site and B-site ordered quadruple perovskite structure. The charge combination is confirmed to be LaMn<sup>3+</sup><sub>3</sub>Ni<sup>2+</sup><sub>2</sub>Mn<sup>4+</sup><sub>2</sub>O<sub>12</sub>, where La and Mn<sup>3+</sup> are 1:3 ordered at the A and Aā€² sites and the Ni<sup>2+</sup> and Mn<sup>4+</sup> are also distributed at the B and Bā€² sites in an orderly fashion in a rocksalt-type manner, respectively. A G-type antiferromagnetic ordering originating from the Aā€²-site Mn<sup>3+</sup> sublattice is found to occur at <i>T</i><sub>N</sub> ā‰ˆ 46 K. Subsequently, the spin coupling between the B-site Ni<sup>2+</sup> and Bā€²-site Mn<sup>4+</sup> sublattices leads to an orthogonally ordered spin alignment with a net ferromagnetic component near <i>T</i><sub>C</sub> ā‰ˆ 34 K. First-principles calculations demonstrate that the Aā€²-site Mn<sup>3+</sup> spins play a crucial role in determining the spin structure of the B and Bā€² sites. This LaMn<sub>3</sub>Ni<sub>2</sub>Mn<sub>2</sub>O<sub>12</sub> provides a rare example that shows orthogonal spin ordering in the B and Bā€² sites assisted by ordered A-site magnetic ions in perovskite systems

    Charge Transfer Induced Multifunctional Transitions with Sensitive Pressure Manipulation in a Metalā€“Organic Framework

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    The metalā€“organic framework {[FeĀ­(2,2ā€²-bipyridine)Ā­(CN)<sub>4</sub>]<sub>2</sub>CoĀ­(4,4ā€²-bipyridine)}Ā·4H<sub>2</sub>O (Fe<sub>2</sub>Co-MOF) with single-chain magnetism undergoes an intermetallic charge transfer that converts the Fe<sub>2</sub>Co charge/spin configurations from Fe<sup>3+</sup><sub>LS</sub>ā€“Co<sup>2+</sup><sub>HS</sub>ā€“Fe<sup>3+</sup><sub>LS</sub> to Fe<sup>2+</sup><sub>LS</sub>ā€“Co<sup>3+</sup><sub>LS</sub>ā€“Fe<sup>3+</sup><sub>LS</sub> (LS = low spin, HS = high spin) around 220 K under ambient pressure. A series of coherent phase transitions in structure, magnetism, permittivity and ferroelectricity are found to take place accompanying with the charge transfer, making Fe<sub>2</sub>Co-MOF a unique ferroelectric single-chain magnet at low temperature. Moreover, our detailed measurements of magnetization, dielectric constant, and Raman scattering under high pressures illustrate that the charge transfer as well as the resulting multifunctional transitions can be readily induced to occur at room temperature by applying a tiny external pressure of about 0.5 kbar. The present study thus provides a pressure well-controllable multifunctional material with potential applications in a broad temperature region across room temperature

    Pressure Induced Amorphization of Pb<sup>2+</sup> and Pb<sup>4+</sup> in Perovskite PbFeO<sub>3</sub>

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    Perovskite-type oxides have been the subject of intense research due to their various fascinating physical properties stemming from their charge degree of freedom. PbFeO3 has an unusual Pb2+0.5Pb4+0.5Fe3+O3 charge distribution with a long-ranged ordering of Pb2+ and Pb4+ and two inequivalent Fe3+ sites in a perovskite structure. Combined synchrotron X-ray diffraction and MoĢˆssbauer spectroscopy revealed a change to an orthorhombic GdFeO3 structure with a unique Fe3+ site and randomly distributed Pb2+ and Pb4+ at 29.0 GPa, namely, pressure-induced amorphization of Pb2+ and Pb4+. The absence of a charge transfer transition to the Pb2+Fe4+O3 phase, which was expected from the comparison with PbCrO3 and PbCoO3, was verified using ab initio density functional theory calculations in the range of 0ā€“70 GPa

    Aā€‘Site and Bā€‘Site Charge Orderings in an <i>sā€“d</i> Level Controlled Perovskite Oxide PbCoO<sub>3</sub>

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    Perovskite PbCoO<sub>3</sub> synthesized at 12 GPa was found to have an unusual charge distribution of Pb<sup>2+</sup>Pb<sup>4+</sup><sub>3</sub>Co<sup>2+</sup><sub>2</sub>Co<sup>3+</sup><sub>2</sub>O<sub>12</sub> with charge orderings in both the A and B sites of perovskite ABO<sub>3</sub>. Comprehensive studies using density functional theory (DFT) calculation, electron diffraction (ED), synchrotron X-ray diffraction (SXRD), neutron powder diffraction (NPD), hard X-ray photoemission spectroscopy (HAXPES), soft X-ray absorption spectroscopy (XAS), and measurements of specific heat as well as magnetic and electrical properties provide evidence of lead ion and cobalt ion charge ordering leading to Pb<sup>2+</sup>Pb<sup>4+</sup><sub>3</sub>Co<sup>2+</sup><sub>2</sub>Co<sup>3+</sup><sub>2</sub>O<sub>12</sub> quadruple perovskite structure. It is shown that the average valence distribution of Pb<sup>3.5+</sup>Co<sup>2.5+</sup>O<sub>3</sub> between Pb<sup>3+</sup>Cr<sup>3+</sup>O<sub>3</sub> and Pb<sup>4+</sup>Ni<sup>2+</sup>O<sub>3</sub> can be stabilized by tuning the energy levels of Pb 6<i>s</i> and transition metal 3<i>d</i> orbitals
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