2015
DOI: 10.1007/s10948-015-3302-4
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Electronic and Magnetic Nano Phase Separation in Cobaltates La2−x Sr x CoO4

Abstract: The single-layer perovskite cobaltates have attracted enormous attention due to the recent observation of hour-glass shaped magnetic excitation spectra which resemble the ones of the famous high-temperature superconducting cuprates. Here, we present an overview of our most recent studies of the spin and charge correlations in floating-zone grown cobaltate single crystals. We find that frustration and a novel kind of electronic and magnetic nano Georg-August-Universitát Göttingen, Institut für Physikalische Che… Show more

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Cited by 11 publications
(8 citation statements)
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“…In materials with regions of short-range atomic order that have different magnetic ground states, the neighboring domains can interact and cause a strong competition between magnetic states in a way that leads to complex magnetic behavior. 31 Such an effect was observed in TlFe 1.6 Se 2 , where a complete spin reorientation is observed in crystals with ordering of Fe vacancies but a competition for moment orientation is observed when nanoscale phase separation exists between atomically ordered and disordered regions. 32 Both Fe 5−x GeTe 2 and TlFe 1.6 Se 2 possess magnetoelastic coupling evidenced by a large lattice response across a magnetic transition, Table 2.…”
Section: B Evolution Of Magnetic Propertiesmentioning
confidence: 86%
“…In materials with regions of short-range atomic order that have different magnetic ground states, the neighboring domains can interact and cause a strong competition between magnetic states in a way that leads to complex magnetic behavior. 31 Such an effect was observed in TlFe 1.6 Se 2 , where a complete spin reorientation is observed in crystals with ordering of Fe vacancies but a competition for moment orientation is observed when nanoscale phase separation exists between atomically ordered and disordered regions. 32 Both Fe 5−x GeTe 2 and TlFe 1.6 Se 2 possess magnetoelastic coupling evidenced by a large lattice response across a magnetic transition, Table 2.…”
Section: B Evolution Of Magnetic Propertiesmentioning
confidence: 86%
“…Indeed, there are similarities between the upper part of the hour-glass magnetic spectrum in La 2−x Sr x CoO 4 and the spectrum in undoped La 2 CoO 4 [21] and also similarities of the lower part of the hour-glass spectrum and half-doped La 1.5 Sr 0.5 CoO 4 [22]. The major difference to conventional phase separation is that the outwards-dispersing branches of the low-energy magnetic excitations are missing (and that energies are renormalized to some extent), i.e., nano phase separation is different from conventional phase separation where the observation of a simple superposition of the magnetic excitation spectra of undoped and half-doped phases would be expected-without any suppression of the outwards-dispersing branches of the low-energy excitations (and without a renormalization of energies) [23].…”
Section: Introductionmentioning
confidence: 94%
“…Besides of a comparative study of Sr 2 RhO 4 single crystals isotypic with Sr 2 RuO 4 mainly polycrystalline Sr 2−x La x RhO 4 samples were studied over a wider doping range x = 0 ∼ 1.0 [9][10][11] . Regarding the recent observations of charge order and nano phase separation in the 3d cobaltate system La 2−x Sr x CoO 4 [12][13][14][15] also the availability of single crystals of the 4d Rhodium analogue with hole-doping levels away from the end member Sr 2 RhO 4 and, especially, around 50% electron doping (Sr 1.5 La 0.5 RhO 4 ), would be of interest for future studies of the charge correlations.…”
Section: Introductionmentioning
confidence: 99%