2016
DOI: 10.1016/j.physe.2016.03.022
|View full text |Cite
|
Sign up to set email alerts
|

Goos–Hänchen shifts in AA-stacked bilayer graphene superlattices

Abstract: The quantum Goos-Hänchen shifts of the transmitted electron beam through an AA-stacked bilayer graphene superlattices is investigated. We found that the band structures of graphene superlattices can have more than one Dirac point, their locations do not depend on the number of barriers. It was revealed that any n-barrier structure is perfectly transparent at normal incidence around the Dirac points created in the superlattices. We showed that the Goos-Hänchen shifts display sharp peaks inside the transmission … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

2
2
0

Year Published

2017
2017
2024
2024

Publication Types

Select...
4
4

Relationship

3
5

Authors

Journals

citations
Cited by 14 publications
(4 citation statements)
references
References 37 publications
(66 reference statements)
2
2
0
Order By: Relevance
“…We observe that the transmission is bilaterally symmetrical with respect to the normal incidence, i.e. k y = 0, and exhibits a behavior similar to that observed for Dirac particle in graphene [24][25][26].…”
Section: Transmission and Conductancesupporting
confidence: 73%
See 1 more Smart Citation
“…We observe that the transmission is bilaterally symmetrical with respect to the normal incidence, i.e. k y = 0, and exhibits a behavior similar to that observed for Dirac particle in graphene [24][25][26].…”
Section: Transmission and Conductancesupporting
confidence: 73%
“…T is plotted for d = 3 Å (red line), 15 Å (blue line), 20 Å (green line), 25 Å (black line) in Figure 4(a) for E = 6 (red line), 7 (blue line) and 8 eV (green line) in Figure 4(b).We observe that the transmission is bilaterally symmetrical with respect to the normal incidence, i.e. k y = 0, and exhibits a behavior similar to that observed for Dirac particle in graphene[24][25][26].It is important to note that in the case of graphene in the absence of a magnetic field, the perfect transmission situation appears very clearly in the case k y = 0 (signature of Klein tunneling), which is not the case in our system made of phosphorene. As shown in Figure4(a), the transmission through thin barriers is negligible compared to that for large d, such behavior is similar to that seen for the transmission thought a single barrier in monolayer phosphorene[20].…”
supporting
confidence: 69%
“…The simplest case is different stacking configurations of bilayer graphene (BLG) which consists of two stacked single layers. Bilayer graphenes have continued to attract significant theoretical interest in recent years [10][11][12][13][14][15][16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%
“…This structure is much more stable and its high-quality samples are developed and studied theoretically and experimentally [9][10][11][12][13]. AA-BLG has a linear energy gapless spectrum with two Dirac cones switched in energy by the quantity γ 1 ≈ 0.2 eV [14], and because of this AA-BLG attained enormous theoretical interest [15][16][17][18][19][20]. Such a structure is expected to be metastable, just lately, stable samples were discovered [21][22][23][24].…”
Section: Introductionmentioning
confidence: 99%