2010
DOI: 10.1021/ja102987d
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Pressure-Induced Spin-State Transition in BiCoO3

Abstract: The structural and electronic properties of BiCoO(3) under high pressure have been investigated. Synchrotron X-ray and neutron powder diffraction studies show that the structure changes from a polar PbTiO(3) type to a centrosymmetric GdFeO(3) type above 3 GPa with a large volume decrease of 13% at room temperature revealing a spin-state change. The first-order transition is accompanied by a drop of electrical resistivity. Structural results show that Co(3+) is present in the low spin state at high pressures, b… Show more

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Cited by 167 publications
(187 citation statements)
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“…26 Moreover, pressure induced structural and spin state phase transitions have also been found in other Co oxides such as BiCoO 3 and SrRu 0.5 Co 0.5 O 3 , etc. 27,28 More recently a pressure induced spin reorientation and spin state transition have been reported in SrCoO 3 . 19 Three spin states have also been reported on Fe sites in CuFeO 2 in rhombohedral and monoclinic phases.…”
Section: Multiferroicsmentioning
confidence: 99%
“…26 Moreover, pressure induced structural and spin state phase transitions have also been found in other Co oxides such as BiCoO 3 and SrRu 0.5 Co 0.5 O 3 , etc. 27,28 More recently a pressure induced spin reorientation and spin state transition have been reported in SrCoO 3 . 19 Three spin states have also been reported on Fe sites in CuFeO 2 in rhombohedral and monoclinic phases.…”
Section: Multiferroicsmentioning
confidence: 99%
“…Many novel phase transitions in perovskite compounds have been thus discovered. For instance, the cubic PbCrO 3 perovskite (Phase I) transforms reversibly to another cubic perovskite (Phase II) with a 9.8% volume collapse at the pressure of ∼1.6 GPa (Xiao et al 2010); the multiferroic material of PbVO 3 , which crystallizes in the polarized tetragonal perovskite (P4mm) structure at ambient conditions, changes reversibly to a cubic perovskite with >10% volume collapse at about 2 GPa (Belik et al 2005); BiCoO 3 has the same polarized structure as PbVO 3 at ambient conditions but transforms to the orthorhombic perovskite (Pnma) with a 13% volume reduction at 3-4 GPa, which is induced by the high-spin to low-spin electronic transition in Co 3+ cation and the complete suppression of the polarized character in the Bi 3+ cation (Oka et al 2010). Silicate perovskites are the primary mineral components in the Earth's lower mantle (Kesson et al 1998;Wood 2000).…”
Section: Introductionmentioning
confidence: 99%
“…The characteristic temperature dependences of the electrical resistivity and the magnetic susceptibility are interpreted as a crossover between the LS state of the (t 2g ) 6 configuration with S = 0 and the HS states of (t 2g ) 4 (e g ) 2 with S = 2. 2) Several exotic phenomena, such as the giant magnetoresistance, 10) magnetic clusters, 11,12) and a ferroelectricity, 14) are attributable to the spin-state change.Correlated electron materials with SSDF is recently reexamined as a plausible candidate of the excitonic insulator (EI). [15][16][17] The EI state has been studied since 1960s in the narrow gap semiconductors and semimetals, [18][19][20][21][22] and is recently reexamined from the modern viewpoints.…”
mentioning
confidence: 99%