Abstract

Expanding the properties of 2D materials and studying strong correlated systems is the focus of many researchers, for which the formation of moiré superlattices can provide access. With periodic moiré patterns, moiré superlattices can induce structural altering and band transformations, resulting in new phenomena including moiré phonons, moiré excitons, topological phase transition, unconventional superconductivity, or Mott insulation. Modulating moiré superlattices through altering twist angles can keep the intrinsic lattices and offer routes to new properties, which is more controllable for property tuning and beneficial for the development of novel physical models and theories. Moiré superlattices have recently become excellent platforms for studying new properties of two-dimensional (2D) layered materials. With periodic moiré patterns, moiré superlattices can induce structural altering and band transformations, resulting in new phenomena including moiré phonons, moiré excitons, topological phase transition, unconventional superconductivity, or Mott insulation. With specific moiré superlattices, bilayer or trilayer 2D materials (including heterostructures) can act as excellent models gathering interlayer interactions, intralayer features, band alignments, charge transport, and other effects (such as spin-orbit coupling and splitting) in a single system. This Review introduces the origin and the modulation of moiré superlattices and summarizes several series of new properties discovered in 2D layered materials. We believe that moiré superlattices mean new access to more structures, more properties, more physics, and more opportunities for both fundamental studies and applications of 2D materials. Moiré superlattices have recently become excellent platforms for studying new properties of two-dimensional (2D) layered materials. With periodic moiré patterns, moiré superlattices can induce structural altering and band transformations, resulting in new phenomena including moiré phonons, moiré excitons, topological phase transition, unconventional superconductivity, or Mott insulation. With specific moiré superlattices, bilayer or trilayer 2D materials (including heterostructures) can act as excellent models gathering interlayer interactions, intralayer features, band alignments, charge transport, and other effects (such as spin-orbit coupling and splitting) in a single system. This Review introduces the origin and the modulation of moiré superlattices and summarizes several series of new properties discovered in 2D layered materials. We believe that moiré superlattices mean new access to more structures, more properties, more physics, and more opportunities for both fundamental studies and applications of 2D materials. Since the successful fabrication of monolayer graphene in 2004, a variety of two-dimensional (2D) layered materials have been obtained and widely used in many fields including electronics, optoelectronics, energy storage, and catalysis.1Zeng M. Xiao Y. Liu J. Yang K. Fu L. Exploring two-dimensional materials toward the next-generation circuits: from monomer design to assembly control.Chem. Rev. 2018; 118: 6236-6296Crossref PubMed Scopus (120) Google Scholar, 2Novoselov K.S. Geim A.K. Morozov S.V. Jiang D. Zhang Y. Dubonos S.V. Grigorieva I.V. Firsov A.A. Electric field effect in atomically thin carbon films.Science. 2004; 306: 666-669Crossref PubMed Scopus (41694) Google Scholar, 3Liu J. Cao H. Jiang B. Xue Y. Fu L. Newborn 2D materials for flexible energy conversion and storage.Sci. 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Compared with other strategies, modulating moiré superlattices of 2D materials and heterostructures indicates the external alteration of each layer rather than the uncontrollable heteroatoms or defects, which tends to keep most of the intrinsic features and induce new properties. This makes it easier to explore more comprehensible and convinced explanations for these phenomena without the interference of structural defects. For homogeneous materials, moiré superlattices are mainly affected by the twist angle, while for heterostructures moiré superlattices highly rely on the twist angle as well as small lattice mismatch. Altering the twist angle can provide a powerful way for the modulation of lattice structures, band structures, and topological properties, and therefore can expand the properties or even create new physics of 2D materials. In addition to interlayer twist angles, moiré superlattices can also be induced by the small lattice mismatch of 2D heterostructures, which can be recognized as the result of electrostatic effects and internal strains of two adjacent layers. Moiré-superlattice-induced properties of 2D materials including graphene,10Lu X. Stepanov P. Yang W. Xie M. Aamir M.A. Das I. Urgell C. Watanabe K. Taniguchi T. Zhang G. et al.Superconductors, orbital magnets and correlated states in magic-angle bilayer graphene.Nature. 2019; 574: 653-657Crossref PubMed Scopus (89) Google Scholar,11Yankowitz M. Chen S. Polshyn H. Zhang Y. Watanabe K. Taniguchi T. Graf D. Young A.F. Dean C.R. Tuning superconductivity in twisted bilayer graphene.Science. 2019; 363: 1059-1064Crossref PubMed Scopus (269) Google Scholar transition metal dichalcogenides (TMDs),12Liu K. Zhang L. Cao T. Jin C. Qiu D. Zhou Q. Zettl A. Yang P. Louie S.G. Wang F. Evolution of interlayer coupling in twisted molybdenum disulfide bilayers.Nat. 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Twistable electronics with dynamically rotatable heterostructures.Science. 2018; 361: 690-693Crossref Scopus (79) Google Scholar have been explored in recent years. Distinct from monolayer 2D materials, moiré superlattices of few-layered materials and heterostructures mainly induce impacts on intralayer structures and properties, which then make it possible to alter the structures and properties of the whole system. Reciprocal lattices of moiré superlattices involved in the system can directly affect the momentum space, and interlayer interactions can alter the phonon modes and charge distribution, which ultimately modulate the band structures, spin states, or topological phases. In other words, moiré superlattices can become an excellent platform for exploring and studying novel phenomena and properties of 2D layered materials, including unconventional superconductivity,17Cao Y. Fatemi V. Demir A. Fang S. Tomarken S.L. Luo J.Y. Sanchez-Yamagishi J.D. Watanabe K. Taniguchi T. 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This paper reviews the innovative access to new properties of 2D layered materials induced by moiré superlattices. Starting with the origin of moiré superlattices, we present the new properties of few-layered graphene, graphene/hexagonal boron nitride (hBN) heterostructures, TMDs, TMD heterostructures, and other material with moiré superlattices. We then introduce how moiré patterns are formed and how to modulate the twist angles. Finally, we summarize the importance of moiré superlattices and demonstrate several challenges existing in the field. We expect that moiré superlattices should provide numerous opportunities to fundamental research and enable 2D materials to exhibit innovative properties and expand the applications. As atomically thin crystals assemble with one another, lattice mismatch and rotation between the layers can lead to different moiré superlattices, which are relevant to twist angles. The angle acts as a pivotal part in the properties of 2D layered materials, especially for van der Waals heterostructures. Recently great breakthroughs have been made in this field, and here we summarize the novel properties of various 2D materials and corresponding heterostructures with moiré patterns. Graphene has become a very flexible platform for engineering novel electronic and optoelectronic properties. Apart from combining graphene with other crystals to construct heterostructures, tuning the rotation angles between layers can also induce new properties and applications. When the layers are rotated to different angles, the periodicity of moiré superlattices will change accordingly, which has a great impact on the electronic structure and interlayer coupling of graphene. For the twisted bilayer graphene (TBG) with small twist angle (no larger than 5°), the interlayer coupling is strong and the Dirac band structure is sensitive to the angles.25Shallcross S. Sharma S. Kandelaki E. Pankratov O.A. Electronic structure of turbostratic graphene.Phys. Rev. B. 2010; 81: 165105Crossref Scopus (224) Google Scholar It is worth mentioning that the moiré band near Fermi energy can be regarded as the flat band when the twist angle is close to the magic angle (Figure 1A),26Bistritzer R. MacDonald A.H. Moiré bands in twisted double-layer graphene.Proc. Natl. Acad. Sci. U S A. 2011; 108: 12233-12237Crossref PubMed Scopus (0) Google Scholar,27Kim K. DaSilva A. Huang S. Fallahazad B. Larentis S. Taniguchi T. Watanabe K. LeRoy B.J. MacDonald A.H. Tutuc E. Tunable moiré bands and strong correlations in small-twist-angle bilayer graphene.Proc. Natl. Acad. Sci. U S A. 2017; 114: 3364-3369Crossref PubMed Scopus (0) Google Scholar and unconventional superconducting can be observed.17Cao Y. Fatemi V. Demir A. Fang S. Tomarken S.L. Luo J.Y. Sanchez-Yamagishi J.D. Watanabe K. Taniguchi T. Kaxiras E. et al.Correlated insulator behaviour at half-filling in magic-angle graphene superlattices.Nature. 2018; 556: 80-84Crossref PubMed Scopus (699) Google Scholar,18Cao Y. Fatemi V. Fang S. Watanabe K. Taniguchi T. Kaxiras E. Jarillo-Herrero P. Unconventional superconductivity in magic-angle graphene superlattices.Nature. 2018; 556: 43-50Crossref PubMed Scopus (1221) Google Scholar At relatively large twist angles (larger than 5°), the interlayer coupling leads to band hybridization away from the Dirac point and results in some novel phenomena. In addition, twisted bilayer-bilayer graphene (TBBG) has also received much attention on account of its correlated insulator states and superconductivity.28Cao Y. Rodan-Legrain D. Rubies-Bigorda O. Park J.M. Watanabe K. Taniguchi T. Jarillo-Herrero P. Tunable correlated states and spin-polarized phases in twisted bilayer–bilayer graphene.Nature. 2020; https://doi.org/10.1038/s41586-020-2260-6Crossref Scopus (16) Google Scholar,29Shen C. 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Tunability of 1/f noise at multiple Dirac cones in hBN encapsulated graphene devices.Nano Lett. 2016; 16: 1042-1049Crossref PubMed Scopus (20) Google Scholar,33Wang L. Zihlmann S. Liu M.-H. Makk P. Watanabe K. Taniguchi T. Baumgartner A. Schönenberger C. New generation of moiré superlattices in doubly aligned hBN/graphene/hBN heterostructures.Nano Lett. 2019; 19: 2371-2376Crossref PubMed Scopus (16) Google Scholar and graphene-black phosphorus (BP).34Liu Y. Rodrigues J.N.B. Luo Y.Z. Li L. Carvalho A. Yang M. Laksono E. Lu J. Bao Y. Xu H. et al.Tailoring sample-wide pseudo-magnetic fields on a graphene–black phosphorus heterostructure.Nat. Nanotechnol. 2018; 13: 828-834Crossref PubMed Scopus (37) Google Scholar In general, these moiré patterns can actuate the band-structure reconstruction and electrical properties of graphene and its heterostructures,35Fang S. Kaxiras E. Electronic structure theory of weakly interacting bilayers.Phys. Rev. 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Early in 2011, Bistritzer and Macdonald established a low-energy continuum model Hamiltonian to study the moiré bands in bilayer graphene.26Bistritzer R. MacDonald A.H. Moiré bands in twisted double-layer graphene.Proc. Natl. Acad. Sci. U S A. 2011; 108: 12233-12237Crossref PubMed Scopus (0) Google Scholar They found that the velocity at the Dirac point is connected with the twist angle (θ), and when θ is close to 1.05° the Fermi velocity is near zero and the moiré band is flat—that is, the theoretically calculated magic angle is the angle at which the Fermi velocity at Dirac points becomes zero, where the electrons move slowly and are localized in the superlattice, resulting in strong correlation.27Kim K. DaSilva A. Huang S. Fallahazad B. Larentis S. Taniguchi T. Watanabe K. LeRoy B.J. MacDonald A.H. Tutuc E. Tunable moiré bands and strong correlations in small-twist-angle bilayer graphene.Proc. Natl. Acad. Sci. U S A. 2017; 114: 3364-3369Crossref PubMed Scopus (0) Google Scholar As shown in Figure 1B,17Cao Y. Fatemi V. Demir A. Fang S. Tomarken S.L. Luo J.Y. Sanchez-Yamagishi J.D. Watanabe K. Taniguchi T. Kaxiras E. et al.Correlated insulator behaviour at half-filling in magic-angle graphene superlattices.Nature. 2018; 556: 80-84Crossref PubMed Scopus (699) Google Scholar two kinds of single-layer graphene Dirac cones are rotated around the Γ point in the Brillouin zone by the twist angle θ. In consideration of the reciprocal lattice of the moiré superlattice, the differences between K and K′ wavevectors cause the mini-Brillouin zone. Besides, Dirac cones near the K or K′ valley partly overlap through interlayer hybridization. As a consequence, such hybridization helps open the energy gap and renormalize the Fermi velocity at Dirac points. To explore temperature dependency, Cao et al. studied the low-temperature conductance of TBG with moiré patterns (θ ≈ 1.08°) as a function of carrier density n (Figure 1C). They discovered a new half-filling insulating state (four electrons for per moiré unit cell), which did not exist in normal graphene. Based on the curves of the temperature-dependent conductance of the corresponding device (Figure 1E), it could be concluded that the superconducting transition temperature is 1.7 K. In addition to temperature, magnetic fields also have an influence on the conductance of half-filling states (Figure 1F). Therefore, unconventional superconducting in TBG superlattice is likely to be linked with the Mott-like state.17Cao Y. Fatemi V. Demir A. Fang S. Tomarken S.L. Luo J.Y. Sanchez-Yamagishi J.D. Watanabe K. Taniguchi T. Kaxiras E. et al.Correlated insulator behaviour at half-filling in magic-angle graphene superlattices.Nature. 2018; 556: 80-84Crossref PubMed Scopus (699) Google Scholar,18Cao Y. Fatemi V. Fang S. Watanabe K. Taniguchi T. Kaxiras E. Jarillo-Herrero P. Unconventional superconductivity in magic-angle graphene superlattices.Nature. 2018; 556: 43-50Crossref PubMed Scopus (1221) Google Scholar Cao et al. demonstrate that there exists a spin-singlet Mott-like insulator ground state when the moiré unit cell is half filled and no external magnetic field is applied. As an external magnetic field is applied, spin polarization and Zeeman splitting contribute to the behavior of superconductivity. However, Padhi et al. considered that the mechanism of unconventional superconducting is closer to Wigner crystallization than Mott insulation.38Padhi B. Setty C. Phillips P.W. Doped twisted bilayer graphene near magic angles: proximity to Wigner crystallization, not Mott insulation.Nano Lett. 2018; 18: 6175-6180Crossref PubMed Scopus (71) Google Scholar Even though the true mechanism of high-temperature superconducting of TBG is still being explored, it is certain that a low-energy flat band induced by rotating the layers by 1.1° contributes to the gate-tunable superconducting and strong correlated insulating phases. In addition to the twist angle, Yankowitz et al. demonstrated that pressure can also tune the superconductivity and correlated insulating phases of TBG, as shown in Figure 1D.11Yankowitz M. Chen S. Polshyn H. Zhang Y. Watanabe K. Taniguchi T. Graf D. Young A.F. Dean C.R. Tuning superconductivity in twisted bilayer graphene.Science. 2019; 363: 1059-1064Crossref PubMed Scopus (269) Google Scholar To sum up, TBG with flat bands is a promising platform for studying other many-body quantum phases and exploring more exotic correlated systems, for example, unconventional superconductors. Apart from superconductivity, the magnetotransport properties of TBG with small twist angles have also attracted much attention. Sharpe et al. presented evidence that a ferromagnetic state can exist in the TBG when the moiré unit cell is three-quarters filled.19Sharpe A.L. Fox E.J. Barnard A.W. Finney J. Watanabe K. Taniguchi T. Kastner M.A. Goldhaber-Gordon D. Emergent ferromagnetism near three-quarters filling in twisted bilayer graphene.Science. 2019; 365: 605-608Crossref PubMed Scopus (130) Google Scholar Magnetotransport in graphene and its heterostructures typically does not rely on the applied external field. However, the researchers found that the transport of three-quarters filled TBG is hysteretic with regard to out-of-plane magnetic field in Figure 2A. As illustrated in Figure 2B, zero-field anomalous Hall resistance acts as the function of the filling of conduction and valence bands. In spite of the observable hysteresis over a wide range of displacement fields, it only appears near three-quarters filling of the mini-Brillouin zone. Recent research on magic-angle TBG has also observed high resistance at three-quarters filling,11Yankowitz M. Chen S. Polshyn H. Zhang Y. Watanabe K. Taniguchi T. Graf D. Young A.F. Dean C.R. Tuning superconductivity in twisted bilayer graphene.Science. 2019; 363: 1059-1064Crossref PubMed Scopus (269) Google Scholar,18Cao Y. Fatemi V. Fang S. Watanabe K. Taniguchi T. Kaxiras E. Jarillo-Herrero P. 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As the twist angle decreased, the photoresponse became weaker and vanished in the gapless case with twist angle less than 0.5°. When the twist angle is larger than 5°, moiré band hybridization of TBG driven by interlayer coupling is away from the Dirac points, leading to other different properties. Many researchers take advantage of van Hove singularity-like electronic resonances to enhance light-matter interactions.49Patel H. Havener R.W. Brown L. Liang Y. Yang L. Park J. Graham M.W. Tunable optical excitations in twisted bilayer graphene form strongly bound excitons.Nano Lett. 2015; 15: 5932-5937Crossref PubMed Scopus (38) Google Scholar, 50Patel H. Huang L. Kim C.-J. Park J. Graham M.W. Stacking angle-tunable photoluminescence from interlayer exciton states in twisted bilayer graphene.Nat. Commun. 2019; 10: 1445Crossref PubMed Scopus (16) Google Scholar, 51Yin J. Wang H. Peng H. Tan Z. Liao L. Lin L. Sun X. Koh A.L. Chen Y. 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