Nontrivial band topology in graphene with nanohole arrays appears periodically with superstructure size m (period 2 for triangular arrays, period 6 for honeycomb arrays).
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Two anomalous acoustic plasmons arise from the geometry of 2D type-II Dirac cones, beyond the conventional sqrt(q) form, with valley-dependent chirality and tunability by gap and substrate.
K intercalation drives a 3D-to-2D electronic crossover in HfTe2 via staging, observed as quantized bilayer/trilayer bands and monolayer-like dispersion in ARPES.
citing papers explorer
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Periodic Behavior of Topology in Graphene with Nanohole Array
Nontrivial band topology in graphene with nanohole arrays appears periodically with superstructure size m (period 2 for triangular arrays, period 6 for honeycomb arrays).
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Anomalous acoustic plasmons in two-dimensional over-tilted Dirac bands
Two anomalous acoustic plasmons arise from the geometry of 2D type-II Dirac cones, beyond the conventional sqrt(q) form, with valley-dependent chirality and tunability by gap and substrate.
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Dimensionality reduction and band quantization induced by potassium intercalation in 1$T$-HfTe$_2$
K intercalation drives a 3D-to-2D electronic crossover in HfTe2 via staging, observed as quantized bilayer/trilayer bands and monolayer-like dispersion in ARPES.