Negative spin Hall magnetoresistance of Pt on the bulk easy-plane antiferromagnet NiO
We report on spin Hall magnetoresistance (SMR) measurements of Pt Hall bars on antiferromagnetic NiO(111) single crystals. An SMR with a sign opposite to conventional SMR is observed over a wide range of temperatures as well as magnetic fields stronger than 0.25 T. The negative sign of the SMR can b...
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creator | Hoogeboom, Geert R. Aqeel, Aisha Kuschel, Timo Palstra, Thomas T. M. van Wees, Bart J. |
description | We report on spin Hall magnetoresistance (SMR) measurements of Pt Hall bars on antiferromagnetic NiO(111) single crystals. An SMR with a sign opposite to conventional SMR is observed over a wide range of temperatures as well as magnetic fields stronger than 0.25 T. The negative sign of the SMR can be explained by the alignment of magnetic moments being almost perpendicular to the external magnetic field within the easy plane (111) of the antiferromagnet. This correlation of magnetic moment alignment and the external magnetic field direction is realized just by the easy-plane nature of the material without the need of any exchange coupling to an additional ferromagnet. The SMR signal strength decreases with increasing temperature, primarily due to the decrease in Néel order by including fluctuations. An increasing magnetic field increases the SMR signal strength as there are fewer domains, and the magnetic moments are more strongly manipulated at high magnetic fields. The SMR is saturated at an applied magnetic field of 6 T, resulting in a spin-mixing conductance of ∼1018 Ω−1 m−2, which is comparable to that of Pt on insulating ferrimagnets such as yttrium iron garnet. An argon plasma treatment doubles the spin-mixing conductance. |
doi_str_mv | 10.1063/1.4997588 |
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M. ; van Wees, Bart J.</creator><creatorcontrib>Hoogeboom, Geert R. ; Aqeel, Aisha ; Kuschel, Timo ; Palstra, Thomas T. M. ; van Wees, Bart J.</creatorcontrib><description>We report on spin Hall magnetoresistance (SMR) measurements of Pt Hall bars on antiferromagnetic NiO(111) single crystals. An SMR with a sign opposite to conventional SMR is observed over a wide range of temperatures as well as magnetic fields stronger than 0.25 T. The negative sign of the SMR can be explained by the alignment of magnetic moments being almost perpendicular to the external magnetic field within the easy plane (111) of the antiferromagnet. This correlation of magnetic moment alignment and the external magnetic field direction is realized just by the easy-plane nature of the material without the need of any exchange coupling to an additional ferromagnet. The SMR signal strength decreases with increasing temperature, primarily due to the decrease in Néel order by including fluctuations. An increasing magnetic field increases the SMR signal strength as there are fewer domains, and the magnetic moments are more strongly manipulated at high magnetic fields. The SMR is saturated at an applied magnetic field of 6 T, resulting in a spin-mixing conductance of ∼1018 Ω−1 m−2, which is comparable to that of Pt on insulating ferrimagnets such as yttrium iron garnet. An argon plasma treatment doubles the spin-mixing conductance.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.4997588</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Alignment ; Antiferromagnetism ; Applied physics ; Argon plasma ; Domains ; Ferrimagnetism ; Ferrimagnets ; Ferromagnetism ; Magnetic fields ; Magnetic moments ; Magnetism ; Magnetoresistance ; Magnetoresistivity ; Nickel oxides ; Resistance ; Signal strength ; Single crystals ; Variation ; Yttrium ; Yttrium-iron garnet</subject><ispartof>Applied physics letters, 2017-07, Vol.111 (5)</ispartof><rights>Author(s)</rights><rights>2017 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c393t-32e205c82448d90bd34198ab8ff847a0d93280b7c386d89cc406a1d2316c2f0e3</citedby><cites>FETCH-LOGICAL-c393t-32e205c82448d90bd34198ab8ff847a0d93280b7c386d89cc406a1d2316c2f0e3</cites><orcidid>0000-0001-6588-9064</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/1.4997588$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,4512,27924,27925,76384</link.rule.ids></links><search><creatorcontrib>Hoogeboom, Geert R.</creatorcontrib><creatorcontrib>Aqeel, Aisha</creatorcontrib><creatorcontrib>Kuschel, Timo</creatorcontrib><creatorcontrib>Palstra, Thomas T. M.</creatorcontrib><creatorcontrib>van Wees, Bart J.</creatorcontrib><title>Negative spin Hall magnetoresistance of Pt on the bulk easy-plane antiferromagnet NiO</title><title>Applied physics letters</title><description>We report on spin Hall magnetoresistance (SMR) measurements of Pt Hall bars on antiferromagnetic NiO(111) single crystals. An SMR with a sign opposite to conventional SMR is observed over a wide range of temperatures as well as magnetic fields stronger than 0.25 T. The negative sign of the SMR can be explained by the alignment of magnetic moments being almost perpendicular to the external magnetic field within the easy plane (111) of the antiferromagnet. This correlation of magnetic moment alignment and the external magnetic field direction is realized just by the easy-plane nature of the material without the need of any exchange coupling to an additional ferromagnet. The SMR signal strength decreases with increasing temperature, primarily due to the decrease in Néel order by including fluctuations. An increasing magnetic field increases the SMR signal strength as there are fewer domains, and the magnetic moments are more strongly manipulated at high magnetic fields. The SMR is saturated at an applied magnetic field of 6 T, resulting in a spin-mixing conductance of ∼1018 Ω−1 m−2, which is comparable to that of Pt on insulating ferrimagnets such as yttrium iron garnet. An argon plasma treatment doubles the spin-mixing conductance.</description><subject>Alignment</subject><subject>Antiferromagnetism</subject><subject>Applied physics</subject><subject>Argon plasma</subject><subject>Domains</subject><subject>Ferrimagnetism</subject><subject>Ferrimagnets</subject><subject>Ferromagnetism</subject><subject>Magnetic fields</subject><subject>Magnetic moments</subject><subject>Magnetism</subject><subject>Magnetoresistance</subject><subject>Magnetoresistivity</subject><subject>Nickel oxides</subject><subject>Resistance</subject><subject>Signal strength</subject><subject>Single crystals</subject><subject>Variation</subject><subject>Yttrium</subject><subject>Yttrium-iron garnet</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp90MtKAzEUBuAgCtbqwjcIuFKYmstckqUUtUJpXdh1yGSSmjpNxiQt9O0dmaILwdXhwHf-Az8A1xhNMCrpPZ7knFcFYydghFFVZRRjdgpGCCGalbzA5-Aixk2_FoTSEVgt9Fomu9cwdtbBmWxbuJVrp5MPOtqYpFMaegNfE_QOpncN6137AbWMh6xrpdNQumSNDsEPd3Bhl5fgzMg26qvjHIPV0-PbdJbNl88v04d5piinKaNEE1QoRvKcNRzVDc0xZ7JmxrC8kqjhlDBUV4qysmFcqRyVEjeE4lIRgzQdg5shtwv-c6djEhu_C65_KQjGJeqLQKxXt4NSwccYtBFdsFsZDgIj8d2awOLYWm_vBhuVTX0x3v3gvQ-_UHSN-Q__Tf4Cntt6Mg</recordid><startdate>20170731</startdate><enddate>20170731</enddate><creator>Hoogeboom, Geert R.</creator><creator>Aqeel, Aisha</creator><creator>Kuschel, Timo</creator><creator>Palstra, Thomas T. M.</creator><creator>van Wees, Bart J.</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/0000-0001-6588-9064</orcidid></search><sort><creationdate>20170731</creationdate><title>Negative spin Hall magnetoresistance of Pt on the bulk easy-plane antiferromagnet NiO</title><author>Hoogeboom, Geert R. ; Aqeel, Aisha ; Kuschel, Timo ; Palstra, Thomas T. M. ; van Wees, Bart J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c393t-32e205c82448d90bd34198ab8ff847a0d93280b7c386d89cc406a1d2316c2f0e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Alignment</topic><topic>Antiferromagnetism</topic><topic>Applied physics</topic><topic>Argon plasma</topic><topic>Domains</topic><topic>Ferrimagnetism</topic><topic>Ferrimagnets</topic><topic>Ferromagnetism</topic><topic>Magnetic fields</topic><topic>Magnetic moments</topic><topic>Magnetism</topic><topic>Magnetoresistance</topic><topic>Magnetoresistivity</topic><topic>Nickel oxides</topic><topic>Resistance</topic><topic>Signal strength</topic><topic>Single crystals</topic><topic>Variation</topic><topic>Yttrium</topic><topic>Yttrium-iron garnet</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hoogeboom, Geert R.</creatorcontrib><creatorcontrib>Aqeel, Aisha</creatorcontrib><creatorcontrib>Kuschel, Timo</creatorcontrib><creatorcontrib>Palstra, Thomas T. M.</creatorcontrib><creatorcontrib>van Wees, Bart J.</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>Hoogeboom, Geert R.</au><au>Aqeel, Aisha</au><au>Kuschel, Timo</au><au>Palstra, Thomas T. M.</au><au>van Wees, Bart J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Negative spin Hall magnetoresistance of Pt on the bulk easy-plane antiferromagnet NiO</atitle><jtitle>Applied physics letters</jtitle><date>2017-07-31</date><risdate>2017</risdate><volume>111</volume><issue>5</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>We report on spin Hall magnetoresistance (SMR) measurements of Pt Hall bars on antiferromagnetic NiO(111) single crystals. An SMR with a sign opposite to conventional SMR is observed over a wide range of temperatures as well as magnetic fields stronger than 0.25 T. The negative sign of the SMR can be explained by the alignment of magnetic moments being almost perpendicular to the external magnetic field within the easy plane (111) of the antiferromagnet. This correlation of magnetic moment alignment and the external magnetic field direction is realized just by the easy-plane nature of the material without the need of any exchange coupling to an additional ferromagnet. The SMR signal strength decreases with increasing temperature, primarily due to the decrease in Néel order by including fluctuations. An increasing magnetic field increases the SMR signal strength as there are fewer domains, and the magnetic moments are more strongly manipulated at high magnetic fields. The SMR is saturated at an applied magnetic field of 6 T, resulting in a spin-mixing conductance of ∼1018 Ω−1 m−2, which is comparable to that of Pt on insulating ferrimagnets such as yttrium iron garnet. An argon plasma treatment doubles the spin-mixing conductance.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4997588</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-6588-9064</orcidid></addata></record> |
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subjects | Alignment Antiferromagnetism Applied physics Argon plasma Domains Ferrimagnetism Ferrimagnets Ferromagnetism Magnetic fields Magnetic moments Magnetism Magnetoresistance Magnetoresistivity Nickel oxides Resistance Signal strength Single crystals Variation Yttrium Yttrium-iron garnet |
title | Negative spin Hall magnetoresistance of Pt on the bulk easy-plane antiferromagnet NiO |
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