Spin-Split Band Hybridization in Graphene Proximitized with α-RuCl 3 Nanosheets
Proximity effects induced in the two-dimensional Dirac material graphene potentially open access to novel and intriguing physical phenomena. Thus far, the coupling between graphene and ferromagnetic insulators has been experimentally established. However, only very little is known about graphene...
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Veröffentlicht in: | Nano letters 2019-07, Vol.19 (7), p.4659-4665 |
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creator | Mashhadi, Soudabeh Kim, Youngwook Kim, Jeongwoo Weber, Daniel Taniguchi, Takashi Watanabe, Kenji Park, Noejung Lotsch, Bettina Smet, Jurgen H Burghard, Marko Kern, Klaus |
description | Proximity effects induced in the two-dimensional Dirac material graphene potentially open access to novel and intriguing physical phenomena. Thus far, the coupling between graphene and ferromagnetic insulators has been experimentally established. However, only very little is known about graphene's interaction with antiferromagnetic insulators. Here, we report a low-temperature study of the electronic properties of high quality van der Waals heterostructures composed of a single graphene layer proximitized with α-RuCl
. The latter is known to become antiferromagnetically ordered below 10 K. Shubnikov-de Haas oscillations in the longitudinal resistance together with Hall resistance measurements provide clear evidence for a band realignment that is accompanied by a transfer of electrons originally occupying the graphene's spin degenerate Dirac cones into α-RuCl
band states with in-plane spin polarization. Left behind are holes in two separate Fermi pockets, only the dispersion of one of which is distorted near the Fermi energy due to spin selective hybridization with these spin polarized α-RuCl
band states. This interpretation is supported by our density functional theory calculations. An unexpected damping of the quantum oscillations as well as a zero-field resistance upturn close to the Néel temperature of α-RuCl
suggest the onset of additional spin scattering due to spin fluctuations in the α-RuCl
. |
doi_str_mv | 10.1021/acs.nanolett.9b01691 |
format | Article |
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. The latter is known to become antiferromagnetically ordered below 10 K. Shubnikov-de Haas oscillations in the longitudinal resistance together with Hall resistance measurements provide clear evidence for a band realignment that is accompanied by a transfer of electrons originally occupying the graphene's spin degenerate Dirac cones into α-RuCl
band states with in-plane spin polarization. Left behind are holes in two separate Fermi pockets, only the dispersion of one of which is distorted near the Fermi energy due to spin selective hybridization with these spin polarized α-RuCl
band states. This interpretation is supported by our density functional theory calculations. An unexpected damping of the quantum oscillations as well as a zero-field resistance upturn close to the Néel temperature of α-RuCl
suggest the onset of additional spin scattering due to spin fluctuations in the α-RuCl
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. The latter is known to become antiferromagnetically ordered below 10 K. Shubnikov-de Haas oscillations in the longitudinal resistance together with Hall resistance measurements provide clear evidence for a band realignment that is accompanied by a transfer of electrons originally occupying the graphene's spin degenerate Dirac cones into α-RuCl
band states with in-plane spin polarization. Left behind are holes in two separate Fermi pockets, only the dispersion of one of which is distorted near the Fermi energy due to spin selective hybridization with these spin polarized α-RuCl
band states. This interpretation is supported by our density functional theory calculations. An unexpected damping of the quantum oscillations as well as a zero-field resistance upturn close to the Néel temperature of α-RuCl
suggest the onset of additional spin scattering due to spin fluctuations in the α-RuCl
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. The latter is known to become antiferromagnetically ordered below 10 K. Shubnikov-de Haas oscillations in the longitudinal resistance together with Hall resistance measurements provide clear evidence for a band realignment that is accompanied by a transfer of electrons originally occupying the graphene's spin degenerate Dirac cones into α-RuCl
band states with in-plane spin polarization. Left behind are holes in two separate Fermi pockets, only the dispersion of one of which is distorted near the Fermi energy due to spin selective hybridization with these spin polarized α-RuCl
band states. This interpretation is supported by our density functional theory calculations. An unexpected damping of the quantum oscillations as well as a zero-field resistance upturn close to the Néel temperature of α-RuCl
suggest the onset of additional spin scattering due to spin fluctuations in the α-RuCl
.</abstract><cop>United States</cop><pmid>31241971</pmid><doi>10.1021/acs.nanolett.9b01691</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0003-4175-9278</orcidid><orcidid>https://orcid.org/0000-0002-4719-8873</orcidid><orcidid>https://orcid.org/0000-0002-3094-303X</orcidid><orcidid>https://orcid.org/0000-0002-7408-7618</orcidid></addata></record> |
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title | Spin-Split Band Hybridization in Graphene Proximitized with α-RuCl 3 Nanosheets |
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