000281111 001__ 281111 000281111 005__ 20250129094354.0 000281111 0247_ $$2doi$$a10.1002/pssr.201510290 000281111 0247_ $$2ISSN$$a1862-6254 000281111 0247_ $$2ISSN$$a1862-6270 000281111 0247_ $$2WOS$$aWOS:000363266800005 000281111 037__ $$aFZJ-2016-00816 000281111 041__ $$aEnglish 000281111 082__ $$a530 000281111 1001_ $$0P:(DE-HGF)0$$aGuo, H.$$b0 000281111 245__ $$aCharge correlations in cobaltates La 2- x Sr x CoO 4 000281111 260__ $$aWeinheim$$bWiley-VCH$$c2015 000281111 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1453384824_2881 000281111 3367_ $$2DataCite$$aOutput Types/Journal article 000281111 3367_ $$00$$2EndNote$$aJournal Article 000281111 3367_ $$2BibTeX$$aARTICLE 000281111 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000281111 3367_ $$2DRIVER$$aarticle 000281111 520__ $$aNano-phase separation in La2–xSrx CoO4 (schematically). Red areas: undoped La2CoO4 islands, blue areas: checkerboard charge ordered regions; black, green and blue balls represent nonmagnetic Co3+ ions, magnetic Co2+ ions and oxygen ions, respectively; green arrows indicate Co2+ spins [1, 2].We report on an elastic neutron scattering study of the charge correlations in La2–xSrx CoO4 with x = 1/3, 0.4 and 0.5. We found that the checkerboard charge ordering correlations present in the x = 0.5 sample persist in the x = 0.4 and 1/3 materials. These checkerboard charge ordering correlations are robust and explain the occurrence of nano-phase separation in layered cobaltates for Sr-concentrations away from half-doping. The half-integer reflections then arise from the nanometer-sized hole-rich regions (blue areas in title figure) instead of the undoped ones (red areas in title figure). The appearance of nano-phase separation is an important ingredient for understanding the formation of hour-glass shaped magnetic excitation spectra in La2–xSrx CoO4. 000281111 536__ $$0G:(DE-HGF)POF3-144$$a144 - Controlling Collective States (POF3-144)$$cPOF3-144$$fPOF III$$x0 000281111 536__ $$0G:(DE-HGF)POF3-524$$a524 - Controlling Collective States (POF3-524)$$cPOF3-524$$fPOF III$$x1 000281111 536__ $$0G:(DE-HGF)POF3-6212$$a6212 - Quantum Condensed Matter: Magnetism, Superconductivity (POF3-621)$$cPOF3-621$$fPOF III$$x2 000281111 536__ $$0G:(DE-HGF)POF3-6213$$a6213 - Materials and Processes for Energy and Transport Technologies (POF3-621)$$cPOF3-621$$fPOF III$$x3 000281111 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x4 000281111 588__ $$aDataset connected to CrossRef 000281111 7001_ $$0P:(DE-Juel1)130944$$aSchmidt, W.$$b1 000281111 7001_ $$0P:(DE-HGF)0$$aTjeng, L. H.$$b2 000281111 7001_ $$0P:(DE-HGF)0$$aKomarek, A. 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