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Unusual magnetic ordering transitions in nanoscale biphasic LuFeO3: the role of the ortho-hexa phase ratio and the local structure

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dc.contributor.author CHATURVEDI, SMITA en_US
dc.contributor.author Shyam, Priyank en_US
dc.contributor.author Shirolkar, Mandar M. en_US
dc.contributor.author KRISHNA, SWATHI S. en_US
dc.contributor.author Sinha, Bhavesh en_US
dc.contributor.author Caliebe, Wolfgang en_US
dc.contributor.author Kalinko, Aleksandr en_US
dc.contributor.author Srinivasan, Gopalan en_US
dc.contributor.author OGALE, SATISHCHANDRA en_US
dc.date.accessioned 2021-01-12T04:00:49Z
dc.date.available 2021-01-12T04:00:49Z
dc.date.issued 2020-12 en_US
dc.identifier.citation Journal of Materials Chemistry C, 8(47), 17000-17008. en_US
dc.identifier.issn 2050-7526 en_US
dc.identifier.issn 2050-7534 en_US
dc.identifier.uri http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5489
dc.identifier.uri https://doi.org/10.1039/D0TC02991B en_US
dc.description.abstract Understanding nanoscale ferromagnetism is becoming increasingly important in view of our enhanced ability to control growth and morphological features of complex nano-systems and their potential translation into emergent high density magnetic device technologies. In this work, we have examined the combined consequences of the magneto-crystalline anisotropy, shape anisotropy, intrinsic phase coexistence, and surface induced self-strain and related anisotropy on the magnetism and magnetic transitions in the case of nanoparticles (NPs) and nanofibers (NFs) of the intriguing multiferroic LuFeO3. We find that the two systems exhibit remarkable differences in the magnetic transitions as well as the value of the canted antiferromagnetic moment by virtue of significant differences in the relative hexagonal (h) and orthorhombic (o) phase contents with the h : o phase contribution in NPs (NFs) being 25 : 75 (77 : 23). In the case of NFs with a major hexagonal component, the bifurcation of ZFC and FC magnetization curves is seen to occur above room temperature with a transition seen at about 150 K, a feature reflecting in-plane (a and b) antiferromagnetic order. In the case of NPs with a dominant o-phase, a weak ferromagnetic (canted antiferromagnetic) signal is noted from 300 K (maximum measurement temperature) down to about 274 K, at which point the antiferromagnetic susceptibility feature is seen. Below 223 K a reentrant ferromagnetic order is seen down to 153 K, at which point a bifurcation is noted between FC and ZFC curves. After subtracting the major component of the field dependent linear moment, the weak ferromagnetic (canted) moment at 300 K is almost 2 orders higher in the case of NFs than NPs. A detailed analysis of phase constitution, local structure and lattice-distortions is performed using X-ray diffraction, Raman spectroscopy, and synchrotron-based X-ray absorption near edge structure (XANES) spectroscopy. The potential significance of the interfaces in influencing the canting via gradient spin order distribution is emphasized. en_US
dc.language.iso en en_US
dc.publisher Royal Society of Chemistry en_US
dc.subject Raman-Scattering en_US
dc.subject 2020 en_US
dc.subject 2021-JAN-WEEK1 en_US
dc.subject TOC-JAN-2021 en_US
dc.title Unusual magnetic ordering transitions in nanoscale biphasic LuFeO3: the role of the ortho-hexa phase ratio and the local structure en_US
dc.type Article en_US
dc.contributor.department Dept. of Physics en_US
dc.identifier.sourcetitle Journal of Materials Chemistry C en_US
dc.publication.originofpublisher Foreign en_US


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