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The unusual magnetism of nanoparticle LaCoO3
Bulk and nanoparticle powders of LaCoO3 (LCO) were synthesized and their magnetic and structural properties were studied using SQUID magnetometry and neutron diffraction. The bulk and large nanoparticles exhibit weak ferromagnetism (FM) below T 85 K and a crossover from strong to weak antiferromagne...
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Published in: | Journal of physics. Condensed matter 2015-05, Vol.27 (17), p.176003-176003 |
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container_end_page | 176003 |
container_issue | 17 |
container_start_page | 176003 |
container_title | Journal of physics. Condensed matter |
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creator | Durand, A M Belanger, D P Hamil, T J Ye, F Chi, S Fernandez-Baca, J A Booth, C H Abdollahian, Y Bhat, M |
description | Bulk and nanoparticle powders of LaCoO3 (LCO) were synthesized and their magnetic and structural properties were studied using SQUID magnetometry and neutron diffraction. The bulk and large nanoparticles exhibit weak ferromagnetism (FM) below T 85 K and a crossover from strong to weak antiferromagnetic (AFM) correlations near a transition expressed in the lattice parameters, To 40 K. This crossover does not occur in the smallest nanoparticles; instead, the magnetic behavior is predominantly ferromagnetic. The amount of FM in the nanoparticles depends on the amount of Co3O4 impurity phase, which induces tensile strain on the LCO lattice. A core-interface model is introduced, with the core region exhibiting the AFM crossover and with FM in the interface region near surfaces and impurity phases. |
doi_str_mv | 10.1088/0953-8984/27/17/176003 |
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(LBNL), Berkeley, CA (United States) ; Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR)</creatorcontrib><description>Bulk and nanoparticle powders of LaCoO3 (LCO) were synthesized and their magnetic and structural properties were studied using SQUID magnetometry and neutron diffraction. The bulk and large nanoparticles exhibit weak ferromagnetism (FM) below T 85 K and a crossover from strong to weak antiferromagnetic (AFM) correlations near a transition expressed in the lattice parameters, To 40 K. This crossover does not occur in the smallest nanoparticles; instead, the magnetic behavior is predominantly ferromagnetic. The amount of FM in the nanoparticles depends on the amount of Co3O4 impurity phase, which induces tensile strain on the LCO lattice. 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The amount of FM in the nanoparticles depends on the amount of Co3O4 impurity phase, which induces tensile strain on the LCO lattice. A core-interface model is introduced, with the core region exhibiting the AFM crossover and with FM in the interface region near surfaces and impurity phases.</description><subject>antiferromagnetism</subject><subject>ferromagnetism</subject><subject>interface effects</subject><subject>magnetism</subject><subject>MATERIALS SCIENCE</subject><subject>nanoparticles</subject><subject>NANOSCIENCE AND NANOTECHNOLOGY</subject><subject>surface effects</subject><issn>0953-8984</issn><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNpt0UtLxDAQB_Agiq6rX2EpXvRg3bwfR1l8wcJeVvAW4jR1I21Tm_bgt7dlVRCEgVx-k2H-g9CC4BuCtV5iI1iujeZLqpZkKokxO0AzwiTJJdcvh2j2i07QaUrvGGOuGT9GJ1RoRQ3FM3S93flsaIY0uCqr3Vvj-5DqLJZZ45rYuq4PUPls7VZxw87QUemq5M-_3zl6vr_brh7z9ebhaXW7zsM4vM8lKYXxxAFlUAIYACUUU9iDpkWpeKEENboQ0hdeS-M1B4adAqw4Vrg0bI4u9v_G1AebIPQedhCbxkNvCZWCaz6iqz1qu_gx-NTbOiTwVeUaH4dkiRxnGsyJGOnimw6vtS9s24XadZ_2J4YRXO5BiK19j0PXjOtZqC1Vlkw1hWvbohwl_UcSbKer2ClwOwX-p5F9AdEjeZc</recordid><startdate>20150508</startdate><enddate>20150508</enddate><creator>Durand, A M</creator><creator>Belanger, D P</creator><creator>Hamil, T J</creator><creator>Ye, F</creator><creator>Chi, S</creator><creator>Fernandez-Baca, J A</creator><creator>Booth, C H</creator><creator>Abdollahian, Y</creator><creator>Bhat, M</creator><general>IOP Publishing</general><scope>NPM</scope><scope>7X8</scope><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>20150508</creationdate><title>The unusual magnetism of nanoparticle LaCoO3</title><author>Durand, A M ; Belanger, D P ; Hamil, T J ; Ye, F ; Chi, S ; Fernandez-Baca, J A ; Booth, C H ; Abdollahian, Y ; Bhat, M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i361t-61f59e1ac23cfcc9cc757370ec82df74d75298d56ede869e84c30a7c074070f93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>antiferromagnetism</topic><topic>ferromagnetism</topic><topic>interface effects</topic><topic>magnetism</topic><topic>MATERIALS SCIENCE</topic><topic>nanoparticles</topic><topic>NANOSCIENCE AND NANOTECHNOLOGY</topic><topic>surface effects</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Durand, A M</creatorcontrib><creatorcontrib>Belanger, D P</creatorcontrib><creatorcontrib>Hamil, T J</creatorcontrib><creatorcontrib>Ye, F</creatorcontrib><creatorcontrib>Chi, S</creatorcontrib><creatorcontrib>Fernandez-Baca, J A</creatorcontrib><creatorcontrib>Booth, C H</creatorcontrib><creatorcontrib>Abdollahian, Y</creatorcontrib><creatorcontrib>Bhat, M</creatorcontrib><creatorcontrib>Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)</creatorcontrib><creatorcontrib>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR)</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Durand, A M</au><au>Belanger, D P</au><au>Hamil, T J</au><au>Ye, F</au><au>Chi, S</au><au>Fernandez-Baca, J A</au><au>Booth, C H</au><au>Abdollahian, Y</au><au>Bhat, M</au><aucorp>Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)</aucorp><aucorp>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The unusual magnetism of nanoparticle LaCoO3</atitle><jtitle>Journal of physics. Condensed matter</jtitle><stitle>JPhysCM</stitle><addtitle>J. Phys.: Condens. Matter</addtitle><date>2015-05-08</date><risdate>2015</risdate><volume>27</volume><issue>17</issue><spage>176003</spage><epage>176003</epage><pages>176003-176003</pages><issn>0953-8984</issn><eissn>1361-648X</eissn><coden>JCOMEL</coden><abstract>Bulk and nanoparticle powders of LaCoO3 (LCO) were synthesized and their magnetic and structural properties were studied using SQUID magnetometry and neutron diffraction. The bulk and large nanoparticles exhibit weak ferromagnetism (FM) below T 85 K and a crossover from strong to weak antiferromagnetic (AFM) correlations near a transition expressed in the lattice parameters, To 40 K. This crossover does not occur in the smallest nanoparticles; instead, the magnetic behavior is predominantly ferromagnetic. The amount of FM in the nanoparticles depends on the amount of Co3O4 impurity phase, which induces tensile strain on the LCO lattice. A core-interface model is introduced, with the core region exhibiting the AFM crossover and with FM in the interface region near surfaces and impurity phases.</abstract><cop>England</cop><pub>IOP Publishing</pub><pmid>25872920</pmid><doi>10.1088/0953-8984/27/17/176003</doi><tpages>7</tpages><oa>free_for_read</oa></addata></record> |
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subjects | antiferromagnetism ferromagnetism interface effects magnetism MATERIALS SCIENCE nanoparticles NANOSCIENCE AND NANOTECHNOLOGY surface effects |
title | The unusual magnetism of nanoparticle LaCoO3 |
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