Advanced Functional Materials · 2018 · 42 citations · 34 references
Natural SciencesMaterials SciencePhysicsMagnetic MaterialsMaterials PhysicsSolid-state ChemistryCrystal ChemistryMagnetic Properties Of SolidsMultiferroic MaterialsPerovskite MaterialsPhase TransitionsRaman SpectroscopyFerroelectric Phase TransitionsFerroelectric PropertiesMagnetic PerovskitesMagnetoelastic CouplingMagnetoelastic StrainOrganic-inorganic Hybrid PerovskitesPerovskite Crystal StructureStrain-mediated Coupling
Abstract Magnetic metal–organic frameworks (MOFs) with a perovskite structure AMX 3 are emerging single‐phased multiferroics with different sources of magnetic and electric ordering. However, the atomic mechanism underlying the multiple ferroic coupling is convincingly clarified. In this work, large single crystals of [(CH 3 ) 2 NH 2 ][Ni(HCOO) 3 ] are synthesized and shown to exhibit a first‐order ferroelectric phase transition at ≈178 K during heating and at ≈151 K during cooling, as confirmed by temperature‐dependent differential scanning calorimetry, Raman scattering, and X‐ray diffraction studies. Resonant ultrasound spectroscopy (RUS) is used to investigate the elastic and anelastic properties between 5 and 300 K. The RUS results show an abrupt disappearance of resonance peaks above the ferroelectric transition point of ≈178 K. This is probably due to the unfreezing of dimethylammonium cation motion which couples with local strain. Small changes in elastic properties associated with two known magnetic transition at ≈35 and ≈15 K, respectively, are indicative of weak magnetoelastic coupling. An apparent peak in acoustic loss accompanying the canted antiferromagnetic ordering (≈35 K) and spin reorientation transition (≈15 K) is attributed to dynamical magnetoelastic coupling on the RUS time scale of ≈10 −6 s. In comparison with the same MOF structures containing Mn 2+ and Co 2+ , the smaller Ni 2+ ions effectively generate an internal chemical pressure and induce a compressed ion force on the anion frameworks. This study opens up a new landscape to explore possibilities for ferroic‐order coupling in molecular MOFs.
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