Transmission electron microscopy and ferromagnetic resonance investigations of tunnel magnetic junctions using Co2MnGe Heusler alloy as magnetic electrodes
HRTEM, nano-beam electronic diffraction, energy dispersive X-rays scanning spectroscopy, Vibrating Sample Magnetometry (VSM) and FerroMagnetic Resonance (FMR) techniques are used in view of comparing (static and dynamic) magnetic and structural properties of Co2MnGe (13 nm)/Al2O3 (3 nm)/Co (13 nm) t...
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description | HRTEM, nano-beam electronic diffraction, energy dispersive X-rays scanning spectroscopy, Vibrating Sample Magnetometry (VSM) and FerroMagnetic Resonance (FMR) techniques are used in view of comparing (static and dynamic) magnetic and structural properties of Co2MnGe (13 nm)/Al2O3 (3 nm)/Co (13 nm) tunnel magnetic junctions (TMJ), deposited on various single crystalline substrates (a-plane sapphire, MgO(100) and Si(111)). They allow for providing a correlation between these magnetic properties and the fine structure investigated at atomic scale. The Al2O3 tunnel barrier is always amorphous and contains a large concentration of Co atoms, which, however, is significantly reduced when using a sapphire substrate. The Co layer is polycrystalline and shows larger grains for films grown on a sapphire substrate. The VSM investigation reveals in-plane anisotropy only for samples grown on a sapphire substrate. The FMR spectra of the TMJs are compared to the obtained ones with a single Co and Co2MnGe films of identical thickness deposited on a sapphire substrate. As expected, two distinct modes are detected in the TMJs while only one mode is observed in each single film. For the TMJ grown on a sapphire substrate the FMR behavior does not significantly differ from the superposition of the individual spectra of the single films, allowing for concluding that the exchange coupling between the two magnetic layers is too small to give rise to observable shifts. For TMJs grown on a Si or on a MgO substrate the resonance spectra reveal one mode which is nearly identical to the obtained one in the single Co film, while the other observed resonance shows a considerably smaller intensity and cannot be described using the magnetic parameters appropriate to the single Co2MnGe film. |
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They allow for providing a correlation between these magnetic properties and the fine structure investigated at atomic scale. The Al2O3 tunnel barrier is always amorphous and contains a large concentration of Co atoms, which, however, is significantly reduced when using a sapphire substrate. The Co layer is polycrystalline and shows larger grains for films grown on a sapphire substrate. The VSM investigation reveals in-plane anisotropy only for samples grown on a sapphire substrate. The FMR spectra of the TMJs are compared to the obtained ones with a single Co and Co2MnGe films of identical thickness deposited on a sapphire substrate. As expected, two distinct modes are detected in the TMJs while only one mode is observed in each single film. For the TMJ grown on a sapphire substrate the FMR behavior does not significantly differ from the superposition of the individual spectra of the single films, allowing for concluding that the exchange coupling between the two magnetic layers is too small to give rise to observable shifts. For TMJs grown on a Si or on a MgO substrate the resonance spectra reveal one mode which is nearly identical to the obtained one in the single Co film, while the other observed resonance shows a considerably smaller intensity and cannot be described using the magnetic parameters appropriate to the single Co2MnGe film.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1311.5589</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Aluminum oxide ; Anisotropy ; Atomic structure ; Ferromagnetic resonance ; Ferromagnetism ; Fine structure ; Heusler alloys ; Magnesium oxide ; Magnetic measurement ; Magnetic properties ; Physics - Materials Science ; Sapphire ; Silicon substrates ; Spectra ; Spectrum analysis ; Superposition (mathematics) ; Thickness ; Transmission electron microscopy</subject><ispartof>arXiv.org, 2013-11</ispartof><rights>2013. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,784,885,27925</link.rule.ids><backlink>$$Uhttps://doi.org/10.48550/arXiv.1311.5589$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1016/j.tsf.2013.11.090$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Belmeguenai, M</creatorcontrib><creatorcontrib>Genevois, C</creatorcontrib><creatorcontrib>Zighem, F</creatorcontrib><creatorcontrib>Roussigné, Y</creatorcontrib><creatorcontrib>S-M, Chérif</creatorcontrib><creatorcontrib>Westerholt, K</creatorcontrib><creatorcontrib>A El Bahoui</creatorcontrib><creatorcontrib>Fnidiki, A</creatorcontrib><creatorcontrib>Moch, P</creatorcontrib><title>Transmission electron microscopy and ferromagnetic resonance investigations of tunnel magnetic junctions using Co2MnGe Heusler alloy as magnetic electrodes</title><title>arXiv.org</title><description>HRTEM, nano-beam electronic diffraction, energy dispersive X-rays scanning spectroscopy, Vibrating Sample Magnetometry (VSM) and FerroMagnetic Resonance (FMR) techniques are used in view of comparing (static and dynamic) magnetic and structural properties of Co2MnGe (13 nm)/Al2O3 (3 nm)/Co (13 nm) tunnel magnetic junctions (TMJ), deposited on various single crystalline substrates (a-plane sapphire, MgO(100) and Si(111)). They allow for providing a correlation between these magnetic properties and the fine structure investigated at atomic scale. The Al2O3 tunnel barrier is always amorphous and contains a large concentration of Co atoms, which, however, is significantly reduced when using a sapphire substrate. The Co layer is polycrystalline and shows larger grains for films grown on a sapphire substrate. The VSM investigation reveals in-plane anisotropy only for samples grown on a sapphire substrate. The FMR spectra of the TMJs are compared to the obtained ones with a single Co and Co2MnGe films of identical thickness deposited on a sapphire substrate. As expected, two distinct modes are detected in the TMJs while only one mode is observed in each single film. For the TMJ grown on a sapphire substrate the FMR behavior does not significantly differ from the superposition of the individual spectra of the single films, allowing for concluding that the exchange coupling between the two magnetic layers is too small to give rise to observable shifts. For TMJs grown on a Si or on a MgO substrate the resonance spectra reveal one mode which is nearly identical to the obtained one in the single Co film, while the other observed resonance shows a considerably smaller intensity and cannot be described using the magnetic parameters appropriate to the single Co2MnGe film.</description><subject>Aluminum oxide</subject><subject>Anisotropy</subject><subject>Atomic structure</subject><subject>Ferromagnetic resonance</subject><subject>Ferromagnetism</subject><subject>Fine structure</subject><subject>Heusler alloys</subject><subject>Magnesium oxide</subject><subject>Magnetic measurement</subject><subject>Magnetic properties</subject><subject>Physics - Materials Science</subject><subject>Sapphire</subject><subject>Silicon substrates</subject><subject>Spectra</subject><subject>Spectrum analysis</subject><subject>Superposition (mathematics)</subject><subject>Thickness</subject><subject>Transmission electron microscopy</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNpFkE9LAzEQxYMgWGrvniTgeWv-brJHKVqFipfelzQ7W1J2k5rsFvtZ_LKmtuhpBub3ZuY9hO4omQstJXk08csd5pRTOpdSV1dowjinhRaM3aBZSjtCCCsVk5JP0Pc6Gp96l5ILHkMHdoi56Z2NIdmwP2LjG9xCjKE3Ww-DszhCCt54C9j5A6TBbc2Q1QmHFg-j99DhP3Y3ensejsn5LV4E9u6XgF9hTB1EbLou5BvpX3H5oYF0i65b0yWYXeoUrV-e14vXYvWxfFs8rQojqSxEu1HGZj8KBNPWCqtI2VjgQirbNszoklVKVhVlWlPYGApWZEhZ07S0AT5F9-e1v8HV--h6E4_1KcD6FGAGHs7APobPMRuud2GMPr9UM6JFqZnmkv8Ad6N4pQ</recordid><startdate>20131121</startdate><enddate>20131121</enddate><creator>Belmeguenai, M</creator><creator>Genevois, C</creator><creator>Zighem, F</creator><creator>Roussigné, Y</creator><creator>S-M, Chérif</creator><creator>Westerholt, K</creator><creator>A El Bahoui</creator><creator>Fnidiki, A</creator><creator>Moch, P</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20131121</creationdate><title>Transmission electron microscopy and ferromagnetic resonance investigations of tunnel magnetic junctions using Co2MnGe Heusler alloy as magnetic electrodes</title><author>Belmeguenai, M ; Genevois, C ; Zighem, F ; Roussigné, Y ; S-M, Chérif ; Westerholt, K ; A El Bahoui ; Fnidiki, A ; Moch, P</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a515-4fb7ac6727e428cc4c706dce3457cfd2a8629759912881eba1ec44c77cadf1de3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Aluminum oxide</topic><topic>Anisotropy</topic><topic>Atomic structure</topic><topic>Ferromagnetic resonance</topic><topic>Ferromagnetism</topic><topic>Fine structure</topic><topic>Heusler alloys</topic><topic>Magnesium oxide</topic><topic>Magnetic measurement</topic><topic>Magnetic properties</topic><topic>Physics - Materials Science</topic><topic>Sapphire</topic><topic>Silicon substrates</topic><topic>Spectra</topic><topic>Spectrum analysis</topic><topic>Superposition (mathematics)</topic><topic>Thickness</topic><topic>Transmission electron microscopy</topic><toplevel>online_resources</toplevel><creatorcontrib>Belmeguenai, M</creatorcontrib><creatorcontrib>Genevois, C</creatorcontrib><creatorcontrib>Zighem, F</creatorcontrib><creatorcontrib>Roussigné, Y</creatorcontrib><creatorcontrib>S-M, Chérif</creatorcontrib><creatorcontrib>Westerholt, K</creatorcontrib><creatorcontrib>A El Bahoui</creatorcontrib><creatorcontrib>Fnidiki, A</creatorcontrib><creatorcontrib>Moch, P</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Belmeguenai, M</au><au>Genevois, C</au><au>Zighem, F</au><au>Roussigné, Y</au><au>S-M, Chérif</au><au>Westerholt, K</au><au>A El Bahoui</au><au>Fnidiki, A</au><au>Moch, P</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Transmission electron microscopy and ferromagnetic resonance investigations of tunnel magnetic junctions using Co2MnGe Heusler alloy as magnetic electrodes</atitle><jtitle>arXiv.org</jtitle><date>2013-11-21</date><risdate>2013</risdate><eissn>2331-8422</eissn><abstract>HRTEM, nano-beam electronic diffraction, energy dispersive X-rays scanning spectroscopy, Vibrating Sample Magnetometry (VSM) and FerroMagnetic Resonance (FMR) techniques are used in view of comparing (static and dynamic) magnetic and structural properties of Co2MnGe (13 nm)/Al2O3 (3 nm)/Co (13 nm) tunnel magnetic junctions (TMJ), deposited on various single crystalline substrates (a-plane sapphire, MgO(100) and Si(111)). They allow for providing a correlation between these magnetic properties and the fine structure investigated at atomic scale. The Al2O3 tunnel barrier is always amorphous and contains a large concentration of Co atoms, which, however, is significantly reduced when using a sapphire substrate. The Co layer is polycrystalline and shows larger grains for films grown on a sapphire substrate. The VSM investigation reveals in-plane anisotropy only for samples grown on a sapphire substrate. The FMR spectra of the TMJs are compared to the obtained ones with a single Co and Co2MnGe films of identical thickness deposited on a sapphire substrate. As expected, two distinct modes are detected in the TMJs while only one mode is observed in each single film. For the TMJ grown on a sapphire substrate the FMR behavior does not significantly differ from the superposition of the individual spectra of the single films, allowing for concluding that the exchange coupling between the two magnetic layers is too small to give rise to observable shifts. For TMJs grown on a Si or on a MgO substrate the resonance spectra reveal one mode which is nearly identical to the obtained one in the single Co film, while the other observed resonance shows a considerably smaller intensity and cannot be described using the magnetic parameters appropriate to the single Co2MnGe film.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1311.5589</doi><oa>free_for_read</oa></addata></record> |
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subjects | Aluminum oxide Anisotropy Atomic structure Ferromagnetic resonance Ferromagnetism Fine structure Heusler alloys Magnesium oxide Magnetic measurement Magnetic properties Physics - Materials Science Sapphire Silicon substrates Spectra Spectrum analysis Superposition (mathematics) Thickness Transmission electron microscopy |
title | Transmission electron microscopy and ferromagnetic resonance investigations of tunnel magnetic junctions using Co2MnGe Heusler alloy as magnetic electrodes |
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