Transition metal partially supported graphene: Magnetism and oscillatory electrostatic potentials
Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of suppo...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Liu, Xiaojie [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2017 |
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| Rechteinformationen: |
Nutzungsrecht: © Author(s) |
|---|
| Übergeordnetes Werk: |
Enthalten in: Journal of applied physics - Melville, NY : AIP, 1937, 122(2017), 5 |
|---|---|
| Übergeordnetes Werk: |
volume:122 ; year:2017 ; number:5 |
| Links: |
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| DOI / URN: |
10.1063/1.4997467 |
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OLC199604513X |
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| 520 | |a Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. | ||
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10.1063/1.4997467 doi PQ20170901 (DE-627)OLC199604513X (DE-599)GBVOLC199604513X (PRQ)scitation_primary_10_1063_1_49974670 (KEY)0076740920170000122000500000transitionmetalpartiallysupportedgraphenemagnetism DE-627 ger DE-627 rakwb eng 530 DE-600 Liu, Xiaojie verfasserin aut Transition metal partially supported graphene: Magnetism and oscillatory electrostatic potentials 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. Nutzungsrecht: © Author(s) Wang, Cai-Zhuang oth Enthalten in Journal of applied physics Melville, NY : AIP, 1937 122(2017), 5 (DE-627)129079030 (DE-600)3112-4 (DE-576)014411652 0021-8979 nnns volume:122 year:2017 number:5 http://dx.doi.org/10.1063/1.4997467 Volltext http://dx.doi.org/10.1063/1.4997467 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_59 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2279 GBV_ILN_4319 AR 122 2017 5 |
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10.1063/1.4997467 doi PQ20170901 (DE-627)OLC199604513X (DE-599)GBVOLC199604513X (PRQ)scitation_primary_10_1063_1_49974670 (KEY)0076740920170000122000500000transitionmetalpartiallysupportedgraphenemagnetism DE-627 ger DE-627 rakwb eng 530 DE-600 Liu, Xiaojie verfasserin aut Transition metal partially supported graphene: Magnetism and oscillatory electrostatic potentials 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. Nutzungsrecht: © Author(s) Wang, Cai-Zhuang oth Enthalten in Journal of applied physics Melville, NY : AIP, 1937 122(2017), 5 (DE-627)129079030 (DE-600)3112-4 (DE-576)014411652 0021-8979 nnns volume:122 year:2017 number:5 http://dx.doi.org/10.1063/1.4997467 Volltext http://dx.doi.org/10.1063/1.4997467 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_59 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2279 GBV_ILN_4319 AR 122 2017 5 |
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10.1063/1.4997467 doi PQ20170901 (DE-627)OLC199604513X (DE-599)GBVOLC199604513X (PRQ)scitation_primary_10_1063_1_49974670 (KEY)0076740920170000122000500000transitionmetalpartiallysupportedgraphenemagnetism DE-627 ger DE-627 rakwb eng 530 DE-600 Liu, Xiaojie verfasserin aut Transition metal partially supported graphene: Magnetism and oscillatory electrostatic potentials 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. Nutzungsrecht: © Author(s) Wang, Cai-Zhuang oth Enthalten in Journal of applied physics Melville, NY : AIP, 1937 122(2017), 5 (DE-627)129079030 (DE-600)3112-4 (DE-576)014411652 0021-8979 nnns volume:122 year:2017 number:5 http://dx.doi.org/10.1063/1.4997467 Volltext http://dx.doi.org/10.1063/1.4997467 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_59 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2279 GBV_ILN_4319 AR 122 2017 5 |
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10.1063/1.4997467 doi PQ20170901 (DE-627)OLC199604513X (DE-599)GBVOLC199604513X (PRQ)scitation_primary_10_1063_1_49974670 (KEY)0076740920170000122000500000transitionmetalpartiallysupportedgraphenemagnetism DE-627 ger DE-627 rakwb eng 530 DE-600 Liu, Xiaojie verfasserin aut Transition metal partially supported graphene: Magnetism and oscillatory electrostatic potentials 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. Nutzungsrecht: © Author(s) Wang, Cai-Zhuang oth Enthalten in Journal of applied physics Melville, NY : AIP, 1937 122(2017), 5 (DE-627)129079030 (DE-600)3112-4 (DE-576)014411652 0021-8979 nnns volume:122 year:2017 number:5 http://dx.doi.org/10.1063/1.4997467 Volltext http://dx.doi.org/10.1063/1.4997467 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_59 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2279 GBV_ILN_4319 AR 122 2017 5 |
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Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. |
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Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. |
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Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. Transition metal partially supported graphene, with a mixture of supported and pristine areas, exhibits an oscillatory electrostatic potential, thus alternating the electric field across the supported and pristine areas. Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a2200265 4500</leader><controlfield tag="001">OLC199604513X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230715064255.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">170901s2017 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1063/1.4997467</subfield><subfield code="2">doi</subfield></datafield><datafield tag="028" ind1="5" ind2="2"><subfield code="a">PQ20170901</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC199604513X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVOLC199604513X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(PRQ)scitation_primary_10_1063_1_49974670</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(KEY)0076740920170000122000500000transitionmetalpartiallysupportedgraphenemagnetism</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Liu, Xiaojie</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Transition metal partially supported graphene: Magnetism and oscillatory electrostatic potentials</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Using first-principles calculations, we show that Mn and Cr layers under graphene exhibit almost zero magnetic moment due to anti-ferromagnetic order, while ferromagnetic coupling in Fe, Co, and Ni leads to large magnetic moment. 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Such an effect can be utilized to control mass transport and nanostructure self-organization on graphene at the atomic level.</subfield></datafield><datafield tag="540" ind1=" " ind2=" "><subfield code="a">Nutzungsrecht: © Author(s)</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wang, Cai-Zhuang</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of applied physics</subfield><subfield code="d">Melville, NY : AIP, 1937</subfield><subfield code="g">122(2017), 5</subfield><subfield code="w">(DE-627)129079030</subfield><subfield code="w">(DE-600)3112-4</subfield><subfield code="w">(DE-576)014411652</subfield><subfield code="x">0021-8979</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:122</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:5</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">http://dx.doi.org/10.1063/1.4997467</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">http://dx.doi.org/10.1063/1.4997467</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_21</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_59</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2279</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4319</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">122</subfield><subfield code="j">2017</subfield><subfield code="e">5</subfield></datafield></record></collection>
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