2023
DOI: 10.48550/arxiv.2301.12234
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Proximity-enhanced valley Zeeman splitting at the WS$_2$/graphene interface

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(6 citation statements)
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“…For the heterostructure bands at the K point, c W(Mo)± , v W(Mo) and v ± , we observe the typical sign changes from R to H stackings because of the opposite K/K (0 • twist) and K/-K (60 • twist) alignment 20,64 . For the conduction bands, we observe deviations of L z on the order of ≤ 0.05 when compared to the monolayer case, consistent with a higher localization of conduction bands 27 . We therefore would expect larger changes arising in the valence bands, which is indeed the case, partic-ularly for the v ± bands, and for the v W and v Mo bands of the H h h stacking.…”
Section: Spin-valley Physics At the Band Edges A Pristine Heterostruc...supporting
confidence: 58%
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“…For the heterostructure bands at the K point, c W(Mo)± , v W(Mo) and v ± , we observe the typical sign changes from R to H stackings because of the opposite K/K (0 • twist) and K/-K (60 • twist) alignment 20,64 . For the conduction bands, we observe deviations of L z on the order of ≤ 0.05 when compared to the monolayer case, consistent with a higher localization of conduction bands 27 . We therefore would expect larger changes arising in the valence bands, which is indeed the case, partic-ularly for the v ± bands, and for the v W and v Mo bands of the H h h stacking.…”
Section: Spin-valley Physics At the Band Edges A Pristine Heterostruc...supporting
confidence: 58%
“…We note that, in order to properly evaluate the intralayer exciton physics, it would be desirable to go beyond DFT calculations and employ the GW + Bethe-Salpeter formalism 45,65,97,125 , which is beyond the scope of this work. Nonetheless, since these intralayer excitons are also quite localized in k-space 10,14,27 , the spin and orbital angular momenta of the Bloch bands should account for the majority of the hybridization effects.…”
Section: Discussionmentioning
confidence: 99%
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