2019
DOI: 10.1134/s0021364019070051
|View full text |Cite
|
Sign up to set email alerts
|

Tunneling in Graphene/h-BN/Graphene Heterostructures through Zero-Dimensional Levels of Defects in h-BN and Their Use as Probes to Measure the Density of States of Graphene

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
6
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 8 publications
(6 citation statements)
references
References 26 publications
0
6
0
Order By: Relevance
“…1 a). This results in single charging behavior characteristic of quantum dots, as seen both in hBN and TMDs 10 , 33 35 . The dimension of a dot embedded within barriers depends on the type of defect and dielectric properties of the medium, and can range from the atomic size to a few nm 34 , 36 .…”
Section: Resultsmentioning
confidence: 98%
“…1 a). This results in single charging behavior characteristic of quantum dots, as seen both in hBN and TMDs 10 , 33 35 . The dimension of a dot embedded within barriers depends on the type of defect and dielectric properties of the medium, and can range from the atomic size to a few nm 34 , 36 .…”
Section: Resultsmentioning
confidence: 98%
“…Similarly, when V g = 1.65 V (blue curve) a peak in the magnitude of the current emerges close to V b = 0. These peaks occur when there is an alignment in energy of the localised state, E 1 , with LLs in the two graphene layers 21 . In effect, the localised state in the hBN barrier acts as a "stepping stone" for electrons tunnelling between the Landau levels of the two graphene electrodes, see inset of Fig.…”
Section: Resultsmentioning
confidence: 99%
“…When the lattices of the graphene layers are aligned so that their relative angular misorientation (twist angle) is small, ≲3°, electrons can tunnel coherently between the Dirac cones of the two layers with the conservation of momentum [8][9][10][11][12][13][14][15] . When the twist angle is large, an electron must scatter in order to tunnel between the misaligned Dirac cones; in this case, tunnelling can occur by phonon-assisted electron tunnelling [16][17][18] or by hopping via defects or impurities within the tunnel barrier [18][19][20][21][22][23][24][25][26] . The large twist angle of ≈30°between the two graphene layers in our devices ensures that direct band-to-band tunnelling with conservation of in-plane momentum is suppressed.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…Coupling defect-dots to source and drain electrodes entails placing an insulating layer between two conductors − the same geometry used for tunnel junctions stacked using the vdW transfer technique 31,32 (Figure 1(a)). This results in single charging behavior characteristic of quantum dots, as seen both in hBN and TMDs 10,[33][34][35] .…”
Section: Defect-assisted Tunneling At Zero Magnetic Fieldmentioning
confidence: 99%