2020
DOI: 10.1002/pssb.202000333
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Electrostatic Detection of Shubnikov–de Haas Oscillations in Bilayer Graphene by Coulomb Resonances in Gate‐Defined Quantum Dots

Abstract: A gate‐defined quantum dot in bilayer graphene is utilized as a sensitive probe for the charge density of its environment. Under the influence of a perpendicular magnetic field, the charge carrier density of the channel region next to the quantum dot oscillates due to the formation of Landau levels. This is experimentally observed as oscillations in the gate‐voltage positions of the Coulomb resonances of the nearby quantum dot. From the frequency of the oscillations, the charge carrier density in the channel i… Show more

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Cited by 12 publications
(9 citation statements)
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“…time in BLG QDs 13 . We therefore apply a finite magnetic field of B ⊥ = 2.4 T to lift the spin and valley degeneracy and, furthermore, to reduce the tunneling rates to the reservoirs 13 , 26 , by altering the density of states in the reservoirs 35 and widening the tunneling barriers. Figure 2 a shows the applied square pulse scheme with amplitude V A and pulse widths τ i and τ m .…”
Section: Resultsmentioning
confidence: 99%
“…time in BLG QDs 13 . We therefore apply a finite magnetic field of B ⊥ = 2.4 T to lift the spin and valley degeneracy and, furthermore, to reduce the tunneling rates to the reservoirs 13 , 26 , by altering the density of states in the reservoirs 35 and widening the tunneling barriers. Figure 2 a shows the applied square pulse scheme with amplitude V A and pulse widths τ i and τ m .…”
Section: Resultsmentioning
confidence: 99%
“…In Fig. 2 tions in the lever-arm, which are due to Shubnikov-de-Haas oscillations in the lead region [24]. With increasing V G , first the GS transition enters the bias window, then additional transitions follow, each appearing as feature of increased differential transconductance, giving rise to a rich spectrum.…”
mentioning
confidence: 96%
“…v )µ B B ⊥ , with the spin g-factor g s = 2, the single-particle (wavefunction dependent) valley g-factor g (1) v and the Bohr magneton µ B [16,[22][23][24]. Note that the valley g-factor is usually around one order of magnitude larger than the spin g-factor.…”
mentioning
confidence: 99%
“…In order to study the spin dynamics of a single-electron in the BLG QD, we now focus on the first charge tran-sition (N = 0 to 1) and apply a perpendicular magnetic field, B ⊥ , to lift the spin and valley degeneracy of the QD and, crucially, to reduce the tunneling rates between the QD and the source-drain reservoirs [14,15,36]. At B ⊥ = 1.5 T, a tunneling current of I ≈ 720 fA at V A = 0 V is observed, corresponding to a combined tunneling rate through the QD of Γ = I/e = Γ L Γ R /(Γ L + Γ R ) ≈ 4.5 MHz.…”
mentioning
confidence: 99%