Abstract:In the magic-angle twisted bilayer graphene (MA-TBG), strong electron-electron (e-e) correlations caused by the band-flattening lead to many exotic quantum phases such as superconductivity, correlated insulator, ferromagnetism, and quantum anomalous Hall effects, when its low-energy van Hove singularities (VHSs) are partially filled. Here our high-resolution scanning tunneling microscope and spectroscopy measurements demonstrate that the e-e correlation in a non-magic-angle TBG with a twist angle θ = 1.49º sti… Show more
“…( 2), the two VHSs move closer to each other with decreasing the twist angles. Here we summarize the energy separations of the two VHSs ∆E VHS vs θ of the TBG acquired from the STS measurements [32,[34][35][36][37][38][39][40][67][68][69][70][71][72]97] as shown in Fig. 2.…”
Section: Symmetry Breaking In the Matbgmentioning
confidence: 99%
“…These parameters are systematically measured by different groups in the past few years. [32][33][34][35][36][37][62][63][64][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79][80][81]126] In Figs. 3(b)-3(e), we summarize the ∆E VHS , the full-width at half-maximum (FWHM) of the VHSs, and the ∆ gap acquired 117303-3 from STS and transport measurements in the TBG near the magic angle, respectively.…”
The electronic properties of van der Waals (vdW) structures can be substantially modified by the moiré superlattice potential, which strongly depends on the twist angle among the compounds. In twisted bilayer graphene (TBG), two low-energy Van Hove singularities (VHSs) move closer with decreasing twist angles and finally become highly non-dispersive flat bands at the magic angle (~ 1.1º). When the Fermi level lies within the flat bands of the TBG near the magic angle, Coulomb interaction is supposed to exceed the kinetic energy of the electrons, which can drive the system into various strongly correlated phases. Moreover, the strongly correlated states of flat bands are also realized in other graphene-based vdW structures with an interlayer twist. In this article, we mainly review the recent experimental advances on the strongly correlated physics of the magic-angle TBG (MATBG) and the small-angle twisted multilayer graphene.Lastly we will give out a perspective of this field.
“…( 2), the two VHSs move closer to each other with decreasing the twist angles. Here we summarize the energy separations of the two VHSs ∆E VHS vs θ of the TBG acquired from the STS measurements [32,[34][35][36][37][38][39][40][67][68][69][70][71][72]97] as shown in Fig. 2.…”
Section: Symmetry Breaking In the Matbgmentioning
confidence: 99%
“…These parameters are systematically measured by different groups in the past few years. [32][33][34][35][36][37][62][63][64][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79][80][81]126] In Figs. 3(b)-3(e), we summarize the ∆E VHS , the full-width at half-maximum (FWHM) of the VHSs, and the ∆ gap acquired 117303-3 from STS and transport measurements in the TBG near the magic angle, respectively.…”
The electronic properties of van der Waals (vdW) structures can be substantially modified by the moiré superlattice potential, which strongly depends on the twist angle among the compounds. In twisted bilayer graphene (TBG), two low-energy Van Hove singularities (VHSs) move closer with decreasing twist angles and finally become highly non-dispersive flat bands at the magic angle (~ 1.1º). When the Fermi level lies within the flat bands of the TBG near the magic angle, Coulomb interaction is supposed to exceed the kinetic energy of the electrons, which can drive the system into various strongly correlated phases. Moreover, the strongly correlated states of flat bands are also realized in other graphene-based vdW structures with an interlayer twist. In this article, we mainly review the recent experimental advances on the strongly correlated physics of the magic-angle TBG (MATBG) and the small-angle twisted multilayer graphene.Lastly we will give out a perspective of this field.
Motivated by measurements of compressibility and STM spectra in twisted bilayer graphene, we analyze the pattern of symmetry breaking for itinerant fermions near a van Hove singularity. Making use of an approximate SU(4) symmetry of the Landau functional, we show that the structure of the spin/isospin order parameter changes with increasing filling via a cascade of transitions. We compute the feedback from different spin/isospin orders on fermions and argue that each order splits the initially 4-fold degenerate van Hove peak in a particular fashion, consistent with the STM data and compressibility measurements, providing a unified interpretation of the cascade of transitions in twisted bilayer graphene. Our results follow from a generic analysis of an SU(4)-symmetric Landau functional and are valid beyond a specific underlying fermionic model. We argue that an analogous van Hove scenario explains the cascade of phase transitions in non-twisted Bernal bilayer and rhombohedral trilayer graphene.
“…Recent developments in the synthesis process have allowed one to obtain a fraction of intermediate twist-angles (down to ∼3°), higher than in previous studies but lacking however deterministic control, as well as moiré transport signatures. To overcome this issue, one can employ a hybrid approach by stacking two CVD-grown SLG to form TBG, obtaining either large or SA twisting, as demonstrated by photoemission − and scanning probe experiments, , respectively. Although permitting high rotational accuracy in analogy to exfoliated flakes, sequentially stacked CVD-grown graphene layers tend to damage and accumulate contaminants at their interface .…”
To realize the applicative
potential of 2D twistronic devices,
scalable synthesis and assembly techniques need to meet stringent
requirements in terms of interface cleanness and twist-angle homogeneity.
Here, we show that small-angle twisted bilayer graphene assembled
from separated CVD-grown graphene single-crystals can ensure high-quality
transport properties, determined by a device-scale-uniform moiré
potential. Via low-temperature dual-gated magnetotransport, we demonstrate
the hallmarks of a 2.4°-twisted superlattice, including tunable
regimes of interlayer coupling, reduced Fermi velocity, large interlayer
capacitance, and density-independent Brown-Zak oscillations. The observation
of these moiré-induced electrical transport features establishes
CVD-based twisted bilayer graphene as an alternative to “tear-and-stack”
exfoliated flakes for fundamental studies, while serving as a proof-of-concept
for future large-scale assembly.
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