5 research outputs found
Strong Magnetocaloric Coupling in Oxyorthosilicate with Dense Gd<sup>3+</sup> Spins
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 3.4 K is derived via the mean-field estimate,
with antiferromagnetic correlations between the ferromagnetically
coupled GdāGd layers. The magnetic entropy change āĪSm is quite impressive, reaches 0.40 J Kā1 cmā3 (58.5 J Kā1 kgā1) 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 ā20 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 BāSite Ordered Quadruple Perovskite with AāSite Tuning Orthogonal Spin Ordering
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 AAā²<sub>3</sub>B<sub>2</sub>Bā²<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 Aā² sites and the Ni<sup>2+</sup> and Mn<sup>4+</sup> are also distributed at the B and Bā²
sites in an orderly fashion in a rocksalt-type manner, respectively.
A G-type antiferromagnetic ordering originating from the Aā²-site
Mn<sup>3+</sup> sublattice is found to occur at <i>T</i><sub>N</sub> ā 46 K. Subsequently, the spin coupling between
the B-site Ni<sup>2+</sup> and Bā²-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 34 K. First-principles
calculations demonstrate that the Aā²-site Mn<sup>3+</sup> spins
play a crucial role in determining the spin structure of the B and
Bā² 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 Bā² sites assisted by ordered A-site magnetic
ions in perovskite systems
Charge Transfer Induced Multifunctional Transitions with Sensitive Pressure Manipulation in a MetalāOrganic Framework
The
metalāorganic framework {[FeĀ(2,2ā²-bipyridine)Ā(CN)<sub>4</sub>]<sub>2</sub>CoĀ(4,4ā²-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>āCo<sup>2+</sup><sub>HS</sub>āFe<sup>3+</sup><sub>LS</sub> to Fe<sup>2+</sup><sub>LS</sub>āCo<sup>3+</sup><sub>LS</sub>āFe<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>
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 MoĢssbauer 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 0ā70 GPa
AāSite and BāSite Charge Orderings in an <i>sād</i> Level Controlled Perovskite Oxide PbCoO<sub>3</sub>
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