2021
DOI: 10.1103/physrevb.103.115425
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Angular momentum anisotropy of Dirac carriers: A new twist in graphene

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Cited by 5 publications
(1 citation statement)
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“…Apart from the Kane–Mele SO coupling, which is intrinsically present in graphene and BLG, extrinsic Bychkov–Rashba SO coupling and pseudospin inversion asymmetry (or principal plane asymmetry) SO coupling can in principle also play a role 12 16 , 28 , 29 . The latter, which arises for example when placing graphene or BLG on substrates, such as e.g., hBN, depends on the magnitude of k (measured from the corners of the Brillouin zone) and is thus suppressed at the and -points 16 , where our devices are operated.…”
Section: Discussionmentioning
confidence: 99%
“…Apart from the Kane–Mele SO coupling, which is intrinsically present in graphene and BLG, extrinsic Bychkov–Rashba SO coupling and pseudospin inversion asymmetry (or principal plane asymmetry) SO coupling can in principle also play a role 12 16 , 28 , 29 . The latter, which arises for example when placing graphene or BLG on substrates, such as e.g., hBN, depends on the magnitude of k (measured from the corners of the Brillouin zone) and is thus suppressed at the and -points 16 , where our devices are operated.…”
Section: Discussionmentioning
confidence: 99%