Cooling field tuned magnetic phase transition and exchange bias-like effect in Y0.9Pr0.1CrO3
Cooling magnetic field dependence of magnetic phase transition has been observed in Y0.9Pr0.1CrO3. GzFx order (spin structure of PrCrO3) is dominant after zero field cooling (ZFC), whereas GxFz order (spin structure of YCrO3) is dominant after cooling under a field higher than 100 Oe. Positive/negat...
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| Veröffentlicht in: | Applied physics letters 2015-09, Vol.107 (10) |
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| container_title | Applied physics letters |
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| creator | Deng, Dongmei Zheng, Jiashun Yu, Dehong Wang, Baomin Sun, Dehui Avdeev, Maxim Feng, Zhenjie Jing, Chao Lu, Bo Ren, Wei Cao, Shixun Zhang, Jincang |
| description | Cooling magnetic field dependence of magnetic phase transition has been observed in Y0.9Pr0.1CrO3. GzFx order (spin structure of PrCrO3) is dominant after zero field cooling (ZFC), whereas GxFz order (spin structure of YCrO3) is dominant after cooling under a field higher than 100 Oe. Positive/negative exchange bias-like effect, with large vertical shift and small horizontal shift, has been observed after FC/ZFC process. The vertical shift can be attributed to the frozen ordered Pr3+ and Cr3+ spins in magnetic domains, because of the strong coupling between Pr3+ and Cr3+ sublattices; while the horizontal shift is a result of the pinning of spins at the interfaces. The frozen structure is generated by the field used for the measurement of the initial magnetization curve of M(H) for the ZFC cooled sample, while it is generated by the cooling field for the sample cooled under a cooling field higher than 100 Oe. |
| doi_str_mv | 10.1063/1.4930302 |
| format | Article |
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GzFx order (spin structure of PrCrO3) is dominant after zero field cooling (ZFC), whereas GxFz order (spin structure of YCrO3) is dominant after cooling under a field higher than 100 Oe. Positive/negative exchange bias-like effect, with large vertical shift and small horizontal shift, has been observed after FC/ZFC process. The vertical shift can be attributed to the frozen ordered Pr3+ and Cr3+ spins in magnetic domains, because of the strong coupling between Pr3+ and Cr3+ sublattices; while the horizontal shift is a result of the pinning of spins at the interfaces. The frozen structure is generated by the field used for the measurement of the initial magnetization curve of M(H) for the ZFC cooled sample, while it is generated by the cooling field for the sample cooled under a cooling field higher than 100 Oe.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.4930302</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Bias ; Cooling ; Cooling effects ; Dependence ; Exchanging ; Lattices (mathematics) ; Magnetic domains ; Magnetism ; Magnetization curves ; Phase transitions ; Spin structure ; Subgroups ; Trivalent chromium</subject><ispartof>Applied physics letters, 2015-09, Vol.107 (10)</ispartof><rights>2015 AIP Publishing LLC.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c323t-4739de9630e4fe2fb11099506fae432a2693af143545073e46f3e767492c14c53</citedby><cites>FETCH-LOGICAL-c323t-4739de9630e4fe2fb11099506fae432a2693af143545073e46f3e767492c14c53</cites><orcidid>0000-0003-0592-9524 ; 0000-0003-2366-5809 ; 0000-0002-3915-2621</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Deng, Dongmei</creatorcontrib><creatorcontrib>Zheng, Jiashun</creatorcontrib><creatorcontrib>Yu, Dehong</creatorcontrib><creatorcontrib>Wang, Baomin</creatorcontrib><creatorcontrib>Sun, Dehui</creatorcontrib><creatorcontrib>Avdeev, Maxim</creatorcontrib><creatorcontrib>Feng, Zhenjie</creatorcontrib><creatorcontrib>Jing, Chao</creatorcontrib><creatorcontrib>Lu, Bo</creatorcontrib><creatorcontrib>Ren, Wei</creatorcontrib><creatorcontrib>Cao, Shixun</creatorcontrib><creatorcontrib>Zhang, Jincang</creatorcontrib><title>Cooling field tuned magnetic phase transition and exchange bias-like effect in Y0.9Pr0.1CrO3</title><title>Applied physics letters</title><description>Cooling magnetic field dependence of magnetic phase transition has been observed in Y0.9Pr0.1CrO3. GzFx order (spin structure of PrCrO3) is dominant after zero field cooling (ZFC), whereas GxFz order (spin structure of YCrO3) is dominant after cooling under a field higher than 100 Oe. Positive/negative exchange bias-like effect, with large vertical shift and small horizontal shift, has been observed after FC/ZFC process. The vertical shift can be attributed to the frozen ordered Pr3+ and Cr3+ spins in magnetic domains, because of the strong coupling between Pr3+ and Cr3+ sublattices; while the horizontal shift is a result of the pinning of spins at the interfaces. The frozen structure is generated by the field used for the measurement of the initial magnetization curve of M(H) for the ZFC cooled sample, while it is generated by the cooling field for the sample cooled under a cooling field higher than 100 Oe.</description><subject>Applied physics</subject><subject>Bias</subject><subject>Cooling</subject><subject>Cooling effects</subject><subject>Dependence</subject><subject>Exchanging</subject><subject>Lattices (mathematics)</subject><subject>Magnetic domains</subject><subject>Magnetism</subject><subject>Magnetization curves</subject><subject>Phase transitions</subject><subject>Spin structure</subject><subject>Subgroups</subject><subject>Trivalent chromium</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNotkE1LAzEYhIMoWD8O_oOAJw9b3-TNZs1RFr-gUA96EIQl3X3Tpm6zNUlB_70r7WkYeJgZhrErAVMBGm_FVBkEBHnEJgKqqkAh7o7ZBACw0KYUp-wspfVoS4k4YZ_1MPQ-LLnz1Hc87wJ1fGOXgbJv-XZlE_EcbUg--yFwGzpOP-3KhiXxhbep6P0XcXKO2sx94B8wNa9xHFPHOV6wE2f7RJcHPWfvjw9v9XMxmz-91PezokWJuVAVmo6MRiDlSLqFEGBMCdpZUiit1AatEwpLVUKFpLRDqnSljGyFaks8Z9f73G0cvneUcrMedjGMlY0UUoERpdIjdbOn2jikFMk12-g3Nv42Apr_8xrRHM7DPxwyXgM</recordid><startdate>20150907</startdate><enddate>20150907</enddate><creator>Deng, Dongmei</creator><creator>Zheng, Jiashun</creator><creator>Yu, Dehong</creator><creator>Wang, Baomin</creator><creator>Sun, Dehui</creator><creator>Avdeev, Maxim</creator><creator>Feng, Zhenjie</creator><creator>Jing, Chao</creator><creator>Lu, Bo</creator><creator>Ren, Wei</creator><creator>Cao, Shixun</creator><creator>Zhang, Jincang</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-0592-9524</orcidid><orcidid>https://orcid.org/0000-0003-2366-5809</orcidid><orcidid>https://orcid.org/0000-0002-3915-2621</orcidid></search><sort><creationdate>20150907</creationdate><title>Cooling field tuned magnetic phase transition and exchange bias-like effect in Y0.9Pr0.1CrO3</title><author>Deng, Dongmei ; Zheng, Jiashun ; Yu, Dehong ; Wang, Baomin ; Sun, Dehui ; Avdeev, Maxim ; Feng, Zhenjie ; Jing, Chao ; Lu, Bo ; Ren, Wei ; Cao, Shixun ; Zhang, Jincang</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c323t-4739de9630e4fe2fb11099506fae432a2693af143545073e46f3e767492c14c53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Applied physics</topic><topic>Bias</topic><topic>Cooling</topic><topic>Cooling effects</topic><topic>Dependence</topic><topic>Exchanging</topic><topic>Lattices (mathematics)</topic><topic>Magnetic domains</topic><topic>Magnetism</topic><topic>Magnetization curves</topic><topic>Phase transitions</topic><topic>Spin structure</topic><topic>Subgroups</topic><topic>Trivalent chromium</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Deng, Dongmei</creatorcontrib><creatorcontrib>Zheng, Jiashun</creatorcontrib><creatorcontrib>Yu, Dehong</creatorcontrib><creatorcontrib>Wang, Baomin</creatorcontrib><creatorcontrib>Sun, Dehui</creatorcontrib><creatorcontrib>Avdeev, Maxim</creatorcontrib><creatorcontrib>Feng, Zhenjie</creatorcontrib><creatorcontrib>Jing, Chao</creatorcontrib><creatorcontrib>Lu, Bo</creatorcontrib><creatorcontrib>Ren, Wei</creatorcontrib><creatorcontrib>Cao, Shixun</creatorcontrib><creatorcontrib>Zhang, Jincang</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Deng, Dongmei</au><au>Zheng, Jiashun</au><au>Yu, Dehong</au><au>Wang, Baomin</au><au>Sun, Dehui</au><au>Avdeev, Maxim</au><au>Feng, Zhenjie</au><au>Jing, Chao</au><au>Lu, Bo</au><au>Ren, Wei</au><au>Cao, Shixun</au><au>Zhang, Jincang</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Cooling field tuned magnetic phase transition and exchange bias-like effect in Y0.9Pr0.1CrO3</atitle><jtitle>Applied physics letters</jtitle><date>2015-09-07</date><risdate>2015</risdate><volume>107</volume><issue>10</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><abstract>Cooling magnetic field dependence of magnetic phase transition has been observed in Y0.9Pr0.1CrO3. GzFx order (spin structure of PrCrO3) is dominant after zero field cooling (ZFC), whereas GxFz order (spin structure of YCrO3) is dominant after cooling under a field higher than 100 Oe. Positive/negative exchange bias-like effect, with large vertical shift and small horizontal shift, has been observed after FC/ZFC process. The vertical shift can be attributed to the frozen ordered Pr3+ and Cr3+ spins in magnetic domains, because of the strong coupling between Pr3+ and Cr3+ sublattices; while the horizontal shift is a result of the pinning of spins at the interfaces. The frozen structure is generated by the field used for the measurement of the initial magnetization curve of M(H) for the ZFC cooled sample, while it is generated by the cooling field for the sample cooled under a cooling field higher than 100 Oe.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4930302</doi><orcidid>https://orcid.org/0000-0003-0592-9524</orcidid><orcidid>https://orcid.org/0000-0003-2366-5809</orcidid><orcidid>https://orcid.org/0000-0002-3915-2621</orcidid></addata></record> |
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| subjects | Applied physics Bias Cooling Cooling effects Dependence Exchanging Lattices (mathematics) Magnetic domains Magnetism Magnetization curves Phase transitions Spin structure Subgroups Trivalent chromium |
| title | Cooling field tuned magnetic phase transition and exchange bias-like effect in Y0.9Pr0.1CrO3 |
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