Emergence of Tertiary Dirac Points in Graphene Moiré Superlattices
The electronic structure of a crystalline solid is largely determined by its lattice structure. Recent advances in van der Waals solids, artificial crystals with controlled stacking of two-dimensional (2D) atomic films, have enabled the creation of materials with novel electronic structures. In part...
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Veröffentlicht in: | Nano letters 2017-06, Vol.17 (6), p.3576-3581 |
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creator | Chen, Guorui Sui, Mengqiao Wang, Duoming Wang, Shuopei Jung, Jeil Moon, Pilkyung Adam, Shaffique Watanabe, Kenji Taniguchi, Takashi Zhou, Shuyun Koshino, Mikito Zhang, Guangyu Zhang, Yuanbo |
description | The electronic structure of a crystalline solid is largely determined by its lattice structure. Recent advances in van der Waals solids, artificial crystals with controlled stacking of two-dimensional (2D) atomic films, have enabled the creation of materials with novel electronic structures. In particular, stacking graphene on hexagonal boron nitride (hBN) introduces a moiré superlattice that fundamentally modifies graphene’s band structure and gives rise to secondary Dirac points (SDPs). Here we find that the formation of a moiré superlattice in graphene on hBN yields new, unexpected consequences: a set of tertiary Dirac points (TDPs) emerge, which give rise to additional sets of Landau levels when the sample is subjected to an external magnetic field. Our observations hint at the formation of a hidden Kekulé superstructure on top of the moiré superlattice under appropriate carrier doping and magnetic fields. |
doi_str_mv | 10.1021/acs.nanolett.7b00735 |
format | Article |
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Recent advances in van der Waals solids, artificial crystals with controlled stacking of two-dimensional (2D) atomic films, have enabled the creation of materials with novel electronic structures. In particular, stacking graphene on hexagonal boron nitride (hBN) introduces a moiré superlattice that fundamentally modifies graphene’s band structure and gives rise to secondary Dirac points (SDPs). Here we find that the formation of a moiré superlattice in graphene on hBN yields new, unexpected consequences: a set of tertiary Dirac points (TDPs) emerge, which give rise to additional sets of Landau levels when the sample is subjected to an external magnetic field. Our observations hint at the formation of a hidden Kekulé superstructure on top of the moiré superlattice under appropriate carrier doping and magnetic fields.</description><identifier>ISSN: 1530-6984</identifier><identifier>EISSN: 1530-6992</identifier><identifier>DOI: 10.1021/acs.nanolett.7b00735</identifier><identifier>PMID: 28475836</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><ispartof>Nano letters, 2017-06, Vol.17 (6), p.3576-3581</ispartof><rights>Copyright © 2017 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a414t-c53552c7ad85119900eb51a1424d224c717282cdd70f4e66f4f4c3c5f558e04a3</citedby><cites>FETCH-LOGICAL-a414t-c53552c7ad85119900eb51a1424d224c717282cdd70f4e66f4f4c3c5f558e04a3</cites><orcidid>0000-0002-4919-4796 ; 0000-0003-3701-8119</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/acs.nanolett.7b00735$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/acs.nanolett.7b00735$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,776,780,2752,27053,27901,27902,56713,56763</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/28475836$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Chen, Guorui</creatorcontrib><creatorcontrib>Sui, Mengqiao</creatorcontrib><creatorcontrib>Wang, Duoming</creatorcontrib><creatorcontrib>Wang, Shuopei</creatorcontrib><creatorcontrib>Jung, Jeil</creatorcontrib><creatorcontrib>Moon, Pilkyung</creatorcontrib><creatorcontrib>Adam, Shaffique</creatorcontrib><creatorcontrib>Watanabe, Kenji</creatorcontrib><creatorcontrib>Taniguchi, Takashi</creatorcontrib><creatorcontrib>Zhou, Shuyun</creatorcontrib><creatorcontrib>Koshino, Mikito</creatorcontrib><creatorcontrib>Zhang, Guangyu</creatorcontrib><creatorcontrib>Zhang, Yuanbo</creatorcontrib><title>Emergence of Tertiary Dirac Points in Graphene Moiré Superlattices</title><title>Nano letters</title><addtitle>Nano Lett</addtitle><description>The electronic structure of a crystalline solid is largely determined by its lattice structure. Recent advances in van der Waals solids, artificial crystals with controlled stacking of two-dimensional (2D) atomic films, have enabled the creation of materials with novel electronic structures. In particular, stacking graphene on hexagonal boron nitride (hBN) introduces a moiré superlattice that fundamentally modifies graphene’s band structure and gives rise to secondary Dirac points (SDPs). Here we find that the formation of a moiré superlattice in graphene on hBN yields new, unexpected consequences: a set of tertiary Dirac points (TDPs) emerge, which give rise to additional sets of Landau levels when the sample is subjected to an external magnetic field. 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Recent advances in van der Waals solids, artificial crystals with controlled stacking of two-dimensional (2D) atomic films, have enabled the creation of materials with novel electronic structures. In particular, stacking graphene on hexagonal boron nitride (hBN) introduces a moiré superlattice that fundamentally modifies graphene’s band structure and gives rise to secondary Dirac points (SDPs). Here we find that the formation of a moiré superlattice in graphene on hBN yields new, unexpected consequences: a set of tertiary Dirac points (TDPs) emerge, which give rise to additional sets of Landau levels when the sample is subjected to an external magnetic field. 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title | Emergence of Tertiary Dirac Points in Graphene Moiré Superlattices |
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