2020
DOI: 10.1103/physrevb.102.085433
|View full text |Cite
|
Sign up to set email alerts
|

Valley current splitter in minimally twisted bilayer graphene

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

1
13
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 21 publications
(14 citation statements)
references
References 37 publications
1
13
0
Order By: Relevance
“…3(c)]. Although the central metallic area is limited enough, the squared modulus of forward propagating wavepacket into terminal 6 is approximately 14%, agreeing well with the result from the Landauer-Büttiker formalism [45], and the rest is equally partitioned towards adjacent terminals 2 and 4. The partition to the adjacent zero lines is well understood due to the overlap between the incoming and outgoing wavefunctions.…”
supporting
confidence: 79%
See 2 more Smart Citations
“…3(c)]. Although the central metallic area is limited enough, the squared modulus of forward propagating wavepacket into terminal 6 is approximately 14%, agreeing well with the result from the Landauer-Büttiker formalism [45], and the rest is equally partitioned towards adjacent terminals 2 and 4. The partition to the adjacent zero lines is well understood due to the overlap between the incoming and outgoing wavefunctions.…”
supporting
confidence: 79%
“…The extremely-high-precision requirement of gating makes the AB-stacked bilayer graphene be challenging in practical application of ZLMs. Fortunately, minimally twisted bilayer graphene provides a natural system in designing ZLM-based electronics [42][43][44][45][46]. However, the physical origin of current partition at the trifurcation point is still unclear, i.e., how can part of the incoming current directly pass through the trifurcation point?…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…There is also a development of a model where a field theoretical approach is applied to the many-body physics of the channel network, but not in a way that leads to specific predictions for the channel states [26]. Finally, in the work by Hou et al [31] a model of the channels is made using a tightbinding model in a single layer graphene with a position-dependent on-site potential; this approach lacks some of the chiral and layer-coupling aspects. All of these models have some limitations; this clearly leaves room for an in depth analysis of the edge states present in a realistic description of such systems.…”
Section: Introductionmentioning
confidence: 99%
“…This can be interpreted as the domain walls acting as links in the network, whereas the AA domains act as nodes. In the valley-protected network, K states arriving at a node have three valley-preserving scattering directions [15,23], as shown in Fig. 2(b).…”
Section: Introductionmentioning
confidence: 99%