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. 2025 Aug 7;25(33):12480–12486. doi: 10.1021/acs.nanolett.5c02309

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(a, b) Experimentally measured transconductance versus B of two QPCs in a WSe2/BLG heterostructure (sample A) at 10 mK. The left QPC (a) is the same device shown in Figure . The right QPC (b) is located on the same heterostructure stack but exhibits a different subband spectrum, likely due to differences in applied gate voltages and possible device-to-device variations. (c, d) Single-particle calculations of QPC energy levels in a BLG/WSe2 heterostructure using DFT SOC parameters from ref with a QPC width of L = 30 nm (left) and L = 50 nm (right). The measured subband evolution, with the states of the first subband highlighted, shows good agreement with theoretical calculations. A notable deviation from the theoretical prediction is marked by an orange circle, indicating a strong bending of the 1K ↓ mode when crossing the 1K+ ↓ mode.