Role of NiO in the nonlocal spin transport through thin NiO films on Y$_3$Fe$_5$O$_{12}
Phys. Rev. B 103, 144406 (2021) In spin transport experiments with spin currents propagating through antiferromagnetic (AFM) material, the antiferromagnet is treated as a mainly passive spin conductor not generating nor adding any spin current to the system. The spin current transmissivity of the AF...
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creator | Hoogeboom, Geert R Nicolaas, Geert-Jan N. Sint Alexander, Andreas Kuschel, Olga Wollschläger, Joachim Ennen, Inga van Wees, Bart J Kuschel, Timo |
description | Phys. Rev. B 103, 144406 (2021) In spin transport experiments with spin currents propagating through
antiferromagnetic (AFM) material, the antiferromagnet is treated as a mainly
passive spin conductor not generating nor adding any spin current to the
system. The spin current transmissivity of the AFM NiO is affected by magnetic
fluctuations, peaking at the N\'eel temperature and decreasing by lowering the
temperature. In order to study the role of the AFM in local and nonlocal spin
transport experiments, we send spin currents through NiO of various thickness
placed on Y$_3$Fe$_5$O$_{12}$. The spin currents are injected either
electrically or by thermal gradients and measured at a wide range of
temperatures and magnetic field strengths. The transmissive role is reflected
in the sign change of the local electrically injected signals and the decrease
in signal strength of all other signals by lowering the temperature. The
thermally generated signals, however, show an additional upturn below 100$\,$K
which are unaffected by an increased NiO thickness. A change in the thermal
conductivity could affect these signals. The temperature and magnetic field
dependence is similar as for bulk NiO, indicating that NiO itself contributes
to thermally induced spin currents. |
doi_str_mv | 10.48550/arxiv.2012.11984 |
format | Article |
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antiferromagnetic (AFM) material, the antiferromagnet is treated as a mainly
passive spin conductor not generating nor adding any spin current to the
system. The spin current transmissivity of the AFM NiO is affected by magnetic
fluctuations, peaking at the N\'eel temperature and decreasing by lowering the
temperature. In order to study the role of the AFM in local and nonlocal spin
transport experiments, we send spin currents through NiO of various thickness
placed on Y$_3$Fe$_5$O$_{12}$. The spin currents are injected either
electrically or by thermal gradients and measured at a wide range of
temperatures and magnetic field strengths. The transmissive role is reflected
in the sign change of the local electrically injected signals and the decrease
in signal strength of all other signals by lowering the temperature. The
thermally generated signals, however, show an additional upturn below 100$\,$K
which are unaffected by an increased NiO thickness. A change in the thermal
conductivity could affect these signals. The temperature and magnetic field
dependence is similar as for bulk NiO, indicating that NiO itself contributes
to thermally induced spin currents.</description><identifier>DOI: 10.48550/arxiv.2012.11984</identifier><language>eng</language><subject>Physics - Materials Science ; Physics - Mesoscale and Nanoscale Physics</subject><creationdate>2020-12</creationdate><rights>http://creativecommons.org/licenses/by-nc-nd/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2012.11984$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2012.11984$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1103/PhysRevB.103.144406$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Hoogeboom, Geert R</creatorcontrib><creatorcontrib>Nicolaas, Geert-Jan N. Sint</creatorcontrib><creatorcontrib>Alexander, Andreas</creatorcontrib><creatorcontrib>Kuschel, Olga</creatorcontrib><creatorcontrib>Wollschläger, Joachim</creatorcontrib><creatorcontrib>Ennen, Inga</creatorcontrib><creatorcontrib>van Wees, Bart J</creatorcontrib><creatorcontrib>Kuschel, Timo</creatorcontrib><title>Role of NiO in the nonlocal spin transport through thin NiO films on Y$_3$Fe$_5$O$_{12}</title><description>Phys. Rev. B 103, 144406 (2021) In spin transport experiments with spin currents propagating through
antiferromagnetic (AFM) material, the antiferromagnet is treated as a mainly
passive spin conductor not generating nor adding any spin current to the
system. The spin current transmissivity of the AFM NiO is affected by magnetic
fluctuations, peaking at the N\'eel temperature and decreasing by lowering the
temperature. In order to study the role of the AFM in local and nonlocal spin
transport experiments, we send spin currents through NiO of various thickness
placed on Y$_3$Fe$_5$O$_{12}$. The spin currents are injected either
electrically or by thermal gradients and measured at a wide range of
temperatures and magnetic field strengths. The transmissive role is reflected
in the sign change of the local electrically injected signals and the decrease
in signal strength of all other signals by lowering the temperature. The
thermally generated signals, however, show an additional upturn below 100$\,$K
which are unaffected by an increased NiO thickness. A change in the thermal
conductivity could affect these signals. The temperature and magnetic field
dependence is similar as for bulk NiO, indicating that NiO itself contributes
to thermally induced spin currents.</description><subject>Physics - Materials Science</subject><subject>Physics - Mesoscale and Nanoscale Physics</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA0NNAzsTA1NdBPLKrILNMzMjA00jM0tLQw4WQID8rPSVXIT1Pwy_RXyMxTKMlIVcjLz8vJT07MUSguAIkUJeYVF-QXlQDlivJL0zOANFAYpD4tMye3WCE_TyFSJd5YxS1VJd5UxV8lvtrQqJaHgTUtMac4lRdKczPIu7mGOHvogp0QX1CUmZtYVBkPcko82CnGhFUAAMbyPJo</recordid><startdate>20201222</startdate><enddate>20201222</enddate><creator>Hoogeboom, Geert R</creator><creator>Nicolaas, Geert-Jan N. Sint</creator><creator>Alexander, Andreas</creator><creator>Kuschel, Olga</creator><creator>Wollschläger, Joachim</creator><creator>Ennen, Inga</creator><creator>van Wees, Bart J</creator><creator>Kuschel, Timo</creator><scope>GOX</scope></search><sort><creationdate>20201222</creationdate><title>Role of NiO in the nonlocal spin transport through thin NiO films on Y$_3$Fe$_5$O$_{12}</title><author>Hoogeboom, Geert R ; Nicolaas, Geert-Jan N. Sint ; Alexander, Andreas ; Kuschel, Olga ; Wollschläger, Joachim ; Ennen, Inga ; van Wees, Bart J ; Kuschel, Timo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_2012_119843</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Physics - Materials Science</topic><topic>Physics - Mesoscale and Nanoscale Physics</topic><toplevel>online_resources</toplevel><creatorcontrib>Hoogeboom, Geert R</creatorcontrib><creatorcontrib>Nicolaas, Geert-Jan N. Sint</creatorcontrib><creatorcontrib>Alexander, Andreas</creatorcontrib><creatorcontrib>Kuschel, Olga</creatorcontrib><creatorcontrib>Wollschläger, Joachim</creatorcontrib><creatorcontrib>Ennen, Inga</creatorcontrib><creatorcontrib>van Wees, Bart J</creatorcontrib><creatorcontrib>Kuschel, Timo</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Hoogeboom, Geert R</au><au>Nicolaas, Geert-Jan N. Sint</au><au>Alexander, Andreas</au><au>Kuschel, Olga</au><au>Wollschläger, Joachim</au><au>Ennen, Inga</au><au>van Wees, Bart J</au><au>Kuschel, Timo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Role of NiO in the nonlocal spin transport through thin NiO films on Y$_3$Fe$_5$O$_{12}</atitle><date>2020-12-22</date><risdate>2020</risdate><abstract>Phys. Rev. B 103, 144406 (2021) In spin transport experiments with spin currents propagating through
antiferromagnetic (AFM) material, the antiferromagnet is treated as a mainly
passive spin conductor not generating nor adding any spin current to the
system. The spin current transmissivity of the AFM NiO is affected by magnetic
fluctuations, peaking at the N\'eel temperature and decreasing by lowering the
temperature. In order to study the role of the AFM in local and nonlocal spin
transport experiments, we send spin currents through NiO of various thickness
placed on Y$_3$Fe$_5$O$_{12}$. The spin currents are injected either
electrically or by thermal gradients and measured at a wide range of
temperatures and magnetic field strengths. The transmissive role is reflected
in the sign change of the local electrically injected signals and the decrease
in signal strength of all other signals by lowering the temperature. The
thermally generated signals, however, show an additional upturn below 100$\,$K
which are unaffected by an increased NiO thickness. A change in the thermal
conductivity could affect these signals. The temperature and magnetic field
dependence is similar as for bulk NiO, indicating that NiO itself contributes
to thermally induced spin currents.</abstract><doi>10.48550/arxiv.2012.11984</doi><oa>free_for_read</oa></addata></record> |
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title | Role of NiO in the nonlocal spin transport through thin NiO films on Y$_3$Fe$_5$O$_{12} |
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