Abstract
Polymorphic structures of transition metal dichalcogenides (TMDs) host exotic electronic states, like charge density wave and superconductivity. However, the number of these structures is limited by crystal symmetries, which poses a challenge to achieving tailored lattices and properties both theoretically and experimentally. Here, we report a coloring-triangle (CT) latticed MoTe2 monolayer, termed CT-MoTe2, constructed by controllably introducing uniform and ordered mirror-twin-boundaries into a pristine monolayer via molecular beam epitaxy. Low-temperature scanning tunneling microscopy and spectroscopy (STM/STS) together with theoretical calculations reveal that the monolayer has an electronic Janus lattice, i.e., an energy-dependent atomic-lattice and a Te pseudo-sublattice, and shares the identical geometry with the Mo5Te8 layer. Dirac-like and flat electronic bands inherently existing in the CT lattice are identified by two broad and two prominent peaks in STS spectra, respectively, and verified with density-functional-theory calculations. Two types of intrinsic domain boundaries were observed, one of which maintains the electronic-Janus-lattice feature, implying potential applications as an energy-tunable electron-tunneling barrier in future functional devices.
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Introduction
Two-dimensional (2D) materials received increasing attention due to their exotic electronic and optical properties1,2,3,4,5,6,7,8,9,10,11,12,13. Recently, it comes into another intriguing property of 2D materials that engineering of their rich polymorphs showing diverse properties for wide applications14,15,16. Polymorph refers to the concept that a given composition with a variety of different crystal structures, including single-element materials and compounds. For instance, borophene possesses a highly polymorphic characteristic. It exhibits many atomic structures due to the complexity of bonding motifs17, in which a series of exotic properties, including massless Dirac fermions18 and 1D nearly free-electron states19, were found. Additional states, such as superconductivity20, charge density wave (CDW)21,22,23, and nontrivial topological states24 were recently found in layered transition metal dichalcogenides (TMDs), offering a particular platform to investigate fundamental condensed matter physics in the two-dimensional limit. Monolayer TMDs were successfully fabricated in many polymorphic phases, such as the hexagonal (1H), octahedral (1 T) and monoclinic (distorted octahedral) (1 T’)25 phases, showing phase-related properties. For example, the monolayer (ML) 1T-NbSe2 exhibits a √13 × √13 CDW order and a correlated magnetic insulating state26, but its 1H counterpart possesses a 3 × 3 CDW order and superconductivity20.
Mirror twin boundaries (MTBs)27,28 were demonstrate to be another strategy to introduce additional exotic electronic states in chalcogen-deficient 1H-MoS229, -MoSe227, and - MoTe230 monolayers. Infinite-length MTBs were theoretically revealed to be metallic and show a high density of states (DOS)31 near the Fermi level (EF). However, they usually exhibit gaps near EF in STS spectra of those monolayers at low temperature, ascribed to the formation of charge orders, like Peierls-type CDW32,33 or Tomonaga-Luttinger liquid34,35. The MTBs, in form of chalcogen-sharing lines, develop in three equivalent zigzag (ZZ) directions of the TMD monolayer lattice. This three-fold equivalence enables the MTBs to form triangular structures and dense networks27, which could serve as block units for potentially building well-defined, like kagome36,37, or coloring-triangle38 lattices. Although it poses a huge challenge to experimental realization, a TMD layer consisting of ordered and uniformly sized MTB triangles, namely an MTB-triangle lattice39,40, could be a TMD phase exhibiting a well-defined lattice symmetry. Therefore, this strategy allows the expansion of the family of polymorphic TMD phases, which are essential for exploring exotic electronic states in the 2D limit.
In this work, we constructed a coloring-triangle (CT) lattice in a MoTe2 (CT-MoTe2) monolayer comprised of uniform-sized and orderly arranged MTB triangular loops and normal MoTe2 domains embedded among MTBs. This CT-MoTe2 monolayer was theoretically proposed and experimentally prepared using a controllable annealing process to an as-grown MoTe2 monolayer. The geometric and electronic structures of CT-MoTe2 were measured using scanning tunneling microscopy/spectroscopy (STM/STS) and verified with first-principles calculations, which reveal an electronic Janus lattice showing two energy-dependent lattices. Further STS measurements in CT-MoTe2 show two prominent peaks near the Fermi level (EF), which are related to two electronic bands inherently existing in CT lattices, as observed in our theoretical calculations. Furthermore, we found a domain boundary in CT-MoTe2, which becomes invisible in certain energy windows. In other words, it behaves like an energy-tunable barrier for electrons flowing through. This work sheds considerable light on the identification of more complicated but uniform polymorphs of TMD monolayers which exhibit exotic electronic phenomena in 2D systems.
Results
Monolayer MoTe2 and MTBs
Figure 1a shows a typical STM topographic image of the MoTe2 sample after post-annealing of an epitaxially grown monolayer on a HOPG substrate at ~513 K. The accompanying STM current image (Fig. 1b) clearly manifests the coexisting of 1H- and 1 T′-MoTe2 phases25. A substantial portion of the 1H regions is covered by high-density mirror-twin boundaries (MTBs), as shown in Fig. 1b and Supplementary Fig. 1, forming various dense MTB networks and/or triangles in different sizes. Figure 1c, d show representative high-resolution topography images of the MTB structures, which appear as single (Fig. 1c) and double (Fig. 1d) bright stripes for the empty and occupied states, respectively. The dI/dV spectra of 1H- and 1 T′-MoTe2, as shown in Fig. 1e and Supplementary Fig. 2d, reveal a semiconducting bandgap of ~1.9 eV, consistent with a previous value of 2.01 eV33, and a semi-metallic gapless feature41, respectively. A distinct narrow U-shaped gap around EF was observed in the dI/dV spectrum acquired on the MTB structure (Fig. 1f), where two sharp peaks residing at the two sides of the gap, ascribed to a Peierls-type CDW32,33 or Tomonaga-Luttinger liquid state34.
The interconnected MTBs of the MoTe2 sample form triangular loop structures surrounding the pristine 1H-MoTe2 domains (Fig. 1d) in which the sizes of the triangles are randomly distributed. Figure 1g–i illustrate the atomic models of three MTB triangles in sizes of N = 1, 3, and 6, where N represents the number of Te2 units (red in Fig. 1g–i) in the 1H-MoTe2 domain. Here, an MTB triangle (highlighted by orange dotted triangles in Fig. 1g–i) contains a Mo-terminated triangular domain (MTTD) of pristine 1H-MoTe2 (highlighted by red hashed triangles in Fig. 1g–i, TeMTTD-R atoms are highlighted by red balls) and its surrounding MTB loops (Te lines). The size of MTTD is governed by the chalcogen deficiency, as demonstrated in the literature30. It was thus an effective route to control the size of MTB triangles that controllably post-growth removal of chalcogen atoms, which was recently achieved by annealing the sample at a certain temperature during a certain period of time27,42,43. In the high MTB density limit, the smallest MTB triangle (N = 1, Fig. 1g) dominantly presents, which, most likely, has a sufficiently large condition window for experimental realization and is expected to host exotic electronic states. We thus use N = 1 MTB triangles (MTTDs) for illustration in our theoretical proposal.
Design and construction of CT-MoTe2 phase
Figure 2a depicts an ordered triangular lattice of the smallest MTTDs, highlighted using red dashed triangles, arranged in a corner-to-edge manner, while blue solid triangles displayed in Fig. 2b highlight a hexagonal lattice of the smallest MTTDs oppositely oriented to the red triangle and assembled in a corner-to-corner manner. Their interstitial regions are filled with the Te lines of MTBs (orange dotted lines in Fig. 2a and b). These MTTDs, together with the MTB loops, form a novel polymorphic MoTe2 phase, the lattice model of which was recently proposed in theory as the coloring-triangular (CT) lattice (Fig. 2c), hosting kagome-like electronic bands38. Thus, we denote this phase as the CT-MoTe2 phase. The CT lattice is a variant of the kagome lattice which is an interesting and well-defined lattice and consists of many sets of two Dirac bands and one flat band. The relationship between the kagome and CT lattices was illustrated in Supplementary Fig. 3.
Density functional theory calculations were further carried out to elucidate the existence of the CT-MoTe2 monolayer. Figure 2d shows the fully relaxed atomic structure of the CT-MoTe2 monolayer, which is, as we proposed, comprised of oppositely oriented N = 1 MTTDs (red and blue triangles) being separated by the MTB loops (Te lines, highlighted by orange dotted triangle). Such an arrangement yields a triangular superlattice with a lattice constant of 12.66 Å (black dashed rhombuses in Fig. 2a–c. However, those central Te atoms of the MTTDs, regardless of their orientations, spatially reside in a smaller triangular lattice with a lattice constant of 7.31 Å. We denote it as the Te pseudo-lattice in the CT-MoTe2 monolayer that its periodicity is expected to show under certain selected energies. This smallest MTB monolayer shares the identical geometry and chemical ratio with the recently found Mo5Te8 monolayer39.
Figure 2e shows the electronic band structure of the CT-MoTe2 monolayer, in which a 0.09 eV energy bandgap opens at the Fermi level. An on-site Coulomb energy U = 1.5 eV is mandatory to obtain this bandgap, suggesting correlated electronic characteristics of the CT-MoTe2 monolayer. Details of U-dependence on the electronic band structures were discussed in Supplementary Fig. 4. There are 12 bands residing near EF, which are categorized into four sets of kagome bands, denoted CT1 to CT4 and coloured in green, blue, violet, and grey, respectively, according to symmetry analysis shown in Supplementary Table I. The irreducible representations (irreps, IRs) of those states at the Γ point were found to be (Γ1, Γ5), (Γ6, Γ2), (Γ3, Γ6), and (Γ5, Γ1), respectively. Thus, sets CT1 (CT2) and CT4 (CT3) are connected through a mirror symmetry operation σh that Γ1 and Γ5 of bands in sets CT1 and CT4 have character 1, while Γ2, Γ3 and Γ6 have character -1 for bands in sets CT2 and CT3. A similar mirror symmetry connection was observable in bands CT1 to CT4 at the K point.
The flat band of CT2 resides at approximately 0.05 eV (over EF, hereinafter), while the all three bands of set CT3 were observable from 0.19 to 0.28 eV in the density of states (DOS) plotted in Fig. 2f, which were denoted states t-S1 and t-S2, respectively. All bands in the green set (CT1) are more dispersive than those in sets CT2 and CT3. The two Dirac-like bands of CT1 show a gap from −0.31 to −0.43 eV, one of which, together with the dispersive “nominal flat band” are observable from −0.02 to −0.37 eV, denoting state t-S0 in Fig. 2g. State t-S3 represent part set CT4 where both the “nominal flat band and the Dirac bands are, again, highly dispersive”. The bands of sets CT1 (green) and CT2 (blue) residing around EF more clearly show the kagome-like features in Fig. 2g and h, which primarily constitute of Te p states and Mo d states. Each set contains a nearly or nominal flat-band and two highly dispersive bands showing Dirac-like behaviors around the K point, although a bandgap opens at K for the CT1 set. Details of these kagome-like bands were discussed in Supplementary Figs. 5 and 6.
We use these two sets for spatial illustration of the CT lattice. We visualized their wavefunction norms of the −0.44 eV (CT1-A) state at the K point and the degenerated states above (−0.32 eV, CT1-B) in Fig. 2i and j, respectively. They, as highlighted using triangles, both show the pattern of the CT lattice. The CT1-A state is partially distributed on the pz states of TeMTTD-R and TeMTB−1 and −4 atoms, while the CT1-B state is comprised of the bonding state of the pxy orbitals of TeMTB−2 and −3 and the pxy state of TeMTTD-B. By this means, CT1-A and CT1-B are energetically and spatially separated. The band structure (Fig. 2h) and visualized wavefunction norms (Fig. 2k and l) of set CT2 exhibit comparable patterns, namely a set of kagome-like bands and CT-symmetry appeared wavefunction norms. However, the contribution from TeMTTD-R nearly eliminates in visualized wavefunction norm of the CT2-A state (0.05 eV) at the K point and those for the TeMTB−1 and −4 atoms are from pxy orbitals (Fig. 2k). Unlike CT1-B, CT2-B is partially constituted of the anti-bonding state of the pxy orbitals of TeMTB−2 and −3 (Fig. 2l), which explains why the CT2 set sits at higher energy and is thus unoccupied. Both pronounced electronic contributions from TeMTTD-R and TeMTTD-B in CT1-A (Fig. 2i), most likely, result in a smaller apparent lattice period of the surface, termed the Te pseudo-sublattice, which is expected to be selectively visualized at certain energy windows. Given the exhibition of the two real-space (quasi-)periodicities, the electronic characteristics of CT-MoTe2 are “double-faced”. We thus termed this feature as the electronic Janus lattice, in which term “Janus” focuses on electronic structures.
An interesting question is thus arisen that whether the kagome-like bands primarily originate from the lattice symmetry, as the in-plane anisotropy of atomic/molecular orbitals on sites of a non-CT or non-kagome lattice may also introduce kagome-like band structures38. Supplementary Fig. 6 shows the frontier orbitals of MTTD and MTB loops involved in forming bands in set CT1 to CT4. Most of these frontier orbitals are comprised of Mo d and Te p orbitals, including the out-of-plane z component and the C3 symmetrized in-plane component, providing identical overlapping matrixes among different sites (Supplementary Fig. 5), which was demonstrated by a tight-binding (TB) d-orbital kagome lattice model intuitively44. Thus, the symmetry of these orbitals guarantees the origin from the lattice symmetry for those kagome-like bands observed in the present work.
Synthesis and characterizations of CT-MoTe2 phase
To experimentally prepare the CT-MoTe2 monolayer, we post-annealed our samples shown in Fig. 1 at an even higher temperature of 616 K. Figure 3a shows a STM topographic image of the sample. Several wire-like features were observed at the edges of the monolayer islands, ascribed to Mo6Te6 nanowires (see Supplementary Fig. 7), clearly demonstrating a phase transition occurred at the edges under a chalcogen-deficient condition45. Moreover, those domains inside the islands show an ordered phase, distinctly different from the 1H- or 1 T′- phase, as locally resolved and marked with white dashed lines in the STM current images (Fig. 3b and Supplementary Fig. 8). A magnified current image (Fig. 3c) more clearly displays the features of the emergent phase, which are consistent with the proposed CT-MoTe2 phase. A structural model of the CT-MoTe2 monolayer was replotted in Fig. 3d where the lattice vectors of the two Janus electronic lattices are displayed in red (atomic-lattice) and blue (Te pseudo-sublattice).
Comparison of a series of bias-dependent experimental (Fig. 3e–h) and theoretical (Fig. 3i–l) STM images verifies that the prepared sample is the CT-MoTe2 monolayer exhibiting the Janus electronic lattices. The experiment and theory are well consistent over a large range of bias voltages in terms of image appearance and apparent lattice periodicity. This series of images shows two apparent lattices, namely a larger one representing the atomic-lattice (red in Fig. 3e–h, a smaller one showing the electronic Te pseudo-sublattice (blue in Fig. 3e and h). The atomic-lattice was exclusively imaged at −0.4 (Fig. 3f) and +0.2 V (Fig. 3g), showing apparent tri-spots features in the 12.2 Å lattice (indicated by the red vectors in Fig. 3e–h). At higher bias voltages, namely −1.3 and +1.5 V, the Te pseudo-sublattice was imaged as bright spots (Fig. 3e) or black pits (Fig. 3h) with a lattice constant of 7.1 Å (indicated by the blue vectors). These two lattices were more straightforwardly illustrated in the FFT images (Supplementary Fig. 9) for those topographic ones shown in Fig. 3e–h. Lattice constants of the both lattices are consistent with the theoretical values of 12.66 and 7.31 Å of the proposed CT-MoTe2 model shown in Fig. 2d. It is also subtly noted that the bright spots in Fig. 3e show a certain chiral characteristic, and one kind of pits (representing TeMTTD-R, denoted using the red circle) appears less dark than the other (TeMTTD-B, the blue circle) in Fig. 3h. These features, consistent with those in the simulated images (Fig. 3i and l), verify again that the prepared sample is the CT-MoTe2 monolayer and indicate the electronic nature of the Te pseudo-sublattice. A similar feature was observed in the Mo5Te8 layer which was, however, inclusively and tentatively assigned to CDW states39,40.
Electronic states of CT-MoTe2 phase
The experimental and theoretical consistency and visualized the appearance of the CT lattice were verified again in Fig. 4. Within an apparent DOS gap (denoted using the green shadow in Fig. 4b) comparable to that of 1H-MoTe2, appreciable in-gap states were observed near the EF (Fig. 4b). A magnified tunneling spectrum of the in-gap states was acquired and plotted in Fig. 4c. It shows a clear dip at EF and two pronounced (e-S1 at 0.05 V and e-S2 at 0.28 V) and two wide peaks (e-S0 spanning from −0.35 – −0.03 V and e-S3 centered at 0.44 V) near the EF. These four peaks were well reproduced in our DOS plot (Fig. 4d) as peaks t-S1 (0.05 eV), t-S2 (0.25 eV), t-S0 (from −0.37 – −0.02 eV), and t-S3 (centered at 0.43 eV). Peak t-S1 originates from state CT2-A, and state t-S2 is contributed from three less dispersive bands of set CT3 (Supplementary Fig. 10). Wide states t-S0 and t-S3 represent the dispersive bands of breathing kagome-like CT1-B (Fig. 2g and j) and CT4 (Supplementary Fig. 10), respectively. These well-consistent assessments indicate the existence of CT and kagome lattices and, at least, one pronounced flat band (CT2-A) that sits only 0.05 eV away from EF and may host strong electron-electron interaction.
Spatial maps of states e-S0 to e-S3 and their corresponding theoretical maps for t-S0 to t-S3 were displayed in Fig. 4e–h and i–l, respectively. The state e-S0 is contributed by dispersive bands CT1-B, which exhibits protrusions around atoms TeMTTD-R and -B in the experimental (Fig. 4e) and theoretical (Fig. 4i) maps. More detailed discussion is supplied in Supplementary Fig. 11. Flat band e-S1 (Fig. 4f), showing a full width at half maximum of ~80 meV, mostly records the spatial distribution of state CT2-A (Figs. 2k and 4j) which exhibits depressions around atoms TeMTTD-R and -B, which were reproduced in the theoretical map (Fig. 4j). For state e-S2 (Fig. 4g), more pronounced charge density was found dominantly around TeMTTD-R (the red circle) than that around TeMTTD-B (the blue circle), well consistent with the theoretical map of t-S2 (Fig. 4k). This map exhibits a lattice of ~12.66 Å, which represents the unit cell of the atomic-lattice. The delocalized e-S3 (t-S3) is mostly distributed on the TeMTB atoms and both the TeMTTD-R and -B atoms appear dark, as shown in Fig. 4h (4 l), which exhibits an electronic lattice of ~7.31 Å (Te pseudo-sublattice). This interesting feature of the electronic Janus lattice in the CT-MoTe2 monolayer was more comprehensively demonstrated in the energy-dependent STM/STS mappings shown in Supplementary Fig. 12.
Discussion
The CT-MoTe2 monolayer, partially constituted of domain boundaries, also has domain boundaries where the electronic Janus lattice feature persists. Figure 5a and b show the STM topography images of a domain boundary acquired at different bias voltages, which exhibits an inversion symmetry of atomic structures and is thus termed the IV boundary of the CT monolayer (DB-IV). DB-IV is characterized by a ZZ-arranged TeMTTD-B atomic chain indicated by light and dark blue triangles and one inversion center was marked using a violet cross in Fig. 5c. In STM images, DB-IV is almost indistinguishable in Fig. 5a where the image exhibits the electronic Te pseudo-sublattice, while it is explicitly imaged in Fig. 5b, in which the atomic-lattice is displayed. These images indicate that the translation symmetry of the atomic-lattice breaks in DB-IV, as plotted in the atomic structure shown in Fig. 5c, but that of the electronic Te pseudo-sublattice is nearly maintained. The energy-dependent continuality of boundary DB-IV could behave like a gate-tunable transport barrier to control flowing of charge carriers across the boundary, as more clearly illustrated in Supplementary Fig. 13. If the CT-MoTe2 was integrated into an electronic device, one would expect DB-IV may promote the gating efficiency at some certain gating voltages. Another example of domain boundaries lies in two TeMTTD-B atomic chains forming a mirror twin (MT) boundary, thus termed DB-MT. We showed its STM images in Fig. 5d and e, while Fig. 5f displays the corresponding atomic structural model. The translation symmetry of either the atomic-lattice or the Te pseudo-sublattice is broken across this boundary, which may lead to emerging properties subject to future experimental and theoretical studies. The feature of DB-IV and DB-MT in the CT-MoTe2 monolayer was more comprehensively demonstrated in the energy-dependent STM images shown in Supplementary Figs. 14 and 15.
In summary, we successfully synthesized the CT-MoTe2 monolayer by introducing the highest MTB density orderly and uniformly into a pristine MoTe2 monolayer using high-temperature post-growth annealing of MBE-grown MoTe2 monolayers. In addition to flat electronic bands and Dirac-like states that the CT lattice symmetry inherently exhibit, the CT-MoTe2 monolayer shows energy-dependent electronic Janus lattices, including the original atomic-lattice and an electronic Te pseudo-sublattice. Two types of domain boundaries were observed in the CT-MoTe2 monolayer, one of which the electronic-Janus-lattice feature maintains implying application potentials in future functional devices. The atomic arrangement of CT-MoTe2 inspires us to further expand the family of polymorphs in CDW phases of TMDs. A straightforward strategy lies in combining honeycomb-arranged CDW units centering an inverted CDW unit in a supercell, whose structural characteristic follows that of the CT-MoTe2 (Supplementary Fig. 16). It was demonstrated that CDW structures in TMDs could be “condensed” selectively by point defects21,46, indicating the above scenario highly promising. Our work offers an effective route to artificially build structural polymorphs in TMDs that host exotic electronic properties to be explored.
Methods
Sample preparation
The single-layer MoTe2 films were grown on highly oriented pyrolytic graphite (HOPG) substrate in a home-built MBE system with a base pressure of 3.0 × 10−10 Torr. The highly oriented pyrolytic graphite (HOPG) substrate was freshly cleaved in air and immediately loaded into the ultra-high vacuum (UHV) chamber of MBE, then degassed at 773 K overnight to remove contaminants. The high-purity Mo (99.999%) and Te (99.999%) were simultaneously evaporated from an electron beam evaporator and a Knudsen cell, respectively. The temperature of HOPG during growth was ~513 K. After growth, all samples were followed by annealing with either a growth temperature maintained or higher temperature (616 K). The sample was monitored by beam flux monitor (BFM) and reflection high-energy electron diffraction (RHEED) to regulate the temperature of both the source and annealing process to form CT-MoTe2 phase.
STM measurements
The samples were transferred to another UHV chamber with LT-STM (PanScan Freedom, RHK) for the following STM measurements. All STM/STS measurements were performed at 9 K with a chemically etched W tip calibrated on a clean Ag(111) surface (Supplementary Fig. 17). The STM images were acquired in constant-current mode. The dI/dV spectra were obtained by using a standard lock-in amplifier with bias modulation ~5 mV at 857 Hz. All STM images were processed by Gwyddion and WSxM47 software.
DFT calculations
Density functional theory calculations were performed using the generalized gradient approximation for the exchange-correlation potential, the projector augmented wave method, and a plane-wave basis set as implemented in the Vienna Ab initio Simulation Package (VASP)48. The energy cutoff for plane wave was set to 500 eV for invariant volume structural relaxation of freestanding CT-MoTe2 monolayers. A dispersion correction was made at the van der Waals density functional (vdW-DF) level, with the optB86b functional for the exchange potential49. During all structural relaxations, all atoms were fully relaxed until the residual force per atom was less than 1 × 10−2 eV Å−1 and the energy convergence criteria was 1 × 10−5 eV. The lattice constant is 12.66 Å after relaxation. The isosurface values for theoretically simulated dI/dV maps are 1 × 10−2 e Bohr−3 and 1 × 10−3 e Bohr−3. A \(7\times 7\times 1\) k-mesh was used to sample the first Brillouin zone in all calculations. An effective on-site Coulomb energy U = 1.5 eV was considered in all calculations. The thickness of the vacuum layer is set to 15 Å. In plotting DOS spectra, a Gaussian smearing of 0.04 eV was used. The energy level of EF was set to energy zero in DOS and band structure calculations.
Data availability
Relevant data supporting the key findings of this study are available within the article and the Supplementary Information file. All raw data generated during the current study are available from the corresponding authors upon request.
References
Wang, Q. H. et al. Electronics and optoelectronics of two-dimensional transition metal dichalcogenides. Nat. Nanotechnol. 7, 699–712 (2012).
Tang, S. et al. Quantum spin Hall state in monolayer 1T′-Wte2. Nat. Phys. 13, 683–687 (2017).
van der Zande, A. M. et al. Grains and grain boundaries in highly crystalline monolayer molybdenum disulphide. Nat. Mater. 12, 554–561 (2013).
Huang, X. et al. Correlated insulating states at fractional fillings of the WS2/Wse2 moiré lattice. Nat. Phys. 17, 715–719 (2021).
Liu, B. et al. Chemical Vapor Deposition Growth of Monolayer Wse2 with Tunable Device Characteristics and Growth Mechanism Study. ACS Nano 9, 6119–6127 (2015).
Zeng, M. et al. Bandgap tuning of two-dimensional materials by sphere diameter engineering. Nat. Mater. 19, 528–533 (2020).
Yuan, S. et al. Room-temperature ferroelectricity in MoTe2 down to the atomic monolayer limit. Nat. Commun. 10, 1775 (2019).
Seo, S.-Y. et al. Writing monolithic integrated circuits on a two-dimensional semiconductor with a scanning light probe. Nat. Electron. 1, 512–517 (2018).
Splendiani, A. et al. Emerging photoluminescence in monolayer MoS2. Nano Lett. 10, 1271–1275 (2010).
Radisavljevic, B. et al. Single-layer MoS2 transistors. Nat. Nanotechnol. 6, 147–150 (2011).
Kuc, A., Zibouche, N. & Heine, T. Influence of quantum confinement on the electronic structure of the transition metal sulfide TaS2. Phys. Rev. B 83, 245213 (2011).
Conley, H. J. et al. Bandgap engineering of strained monolayer and bilayer MoS2. Nano Lett. 13, 3626–3630 (2013).
Xing, S. Y. et al. Interweaving Polar Charge Orders in a Layered Metallic Superatomic Crystal. Phys. Rev. X 12, 041034 (2022).
Wu, M. et al. Nine new phosphorene polymorphs with non-honeycomb structures: a much extended family. Nano Lett. 15, 3557–3562 (2015).
Li, Q. et al. Synthesis of borophane polymorphs through hydrogenation of borophene. Science 371, 1143–1148 (2021).
Feng, B. et al. Experimental realization of two-dimensional boron sheets. Nat. Chem. 8, 563–568 (2016).
Wu, X. et al. Two-Dimensional Boron Monolayer Sheets. ACS Nano 6, 7443–7453 (2012).
Feng, B. et al. Dirac Fermions in Borophene. Phys. Rev. Lett. 118, 096401 (2017).
Kong, L. et al. One-dimensional nearly free electron states in borophene. Nanoscale 11, 15605–15611 (2019).
Ugeda, M. M. et al. Characterization of collective ground states in single-layer NbSe2. Nat. Phys. 12, 92–97 (2015).
Oh, E., Gye, G. & Yeom, H. W. Defect-Selective Charge-Density-Wave Condensation in 2H-NbSe2. Phys. Rev. Lett. 125, 036804 (2020).
Yu, Y. et al. Gate-tunable phase transitions in thin flakes of 1T-TaS2. Nat. Nanotechnol. 10, 270–276 (2015).
Wang, Y. D. et al. Band insulator to Mott insulator transition in 1T-TaS2. Nat. Commun. 11, 4215 (2020).
Jia, Z. Y. et al. Direct visualization of a two-dimensional topological insulator in the single-layer 1T′−WTe2. Phys. Rev. B 96, 041108 (2017).
Duerloo, K. A., Li, Y. & Reed, E. J. Structural phase transitions in two-dimensional Mo- and W-dichalcogenide monolayers. Nat. Commun. 5, 4214 (2014).
Liu, L. et al. Direct identification of Mott Hubbard band pattern beyond charge density wave superlattice in monolayer 1T-NbSe2. Nat. Commun. 12, 1978 (2021).
Liu, H. et al. Dense network of one-dimensional midgap metallic modes in monolayer MoSe2 and their spatial undulations. Phys. Rev. Lett. 113, 066105 (2014).
Hong, J. et al. Inversion Domain Boundary Induced Stacking and Band structure Diversity in Bilayer MoSe2. Nano Lett. 17, 6653–6660 (2017).
Zhou, W. et al. Intrinsic structural defects in monolayer molybdenum disulfide. Nano Lett. 13, 2615–2622 (2013).
Diaz, H. C. et al. High density of (pseudo) periodic twin-grain boundaries in molecular beam epitaxy-grown van der Waals heterostructure: MoTe2/MoS2. Appl. Phys. Lett. 108, 191606 (2016).
Lehtinen, O. et al. Atomic scale microstructure and properties of Se-deficient two-dimensional MoSe2. ACS Nano 9, 3274–3283 (2015).
Barja, S. et al. Charge density wave order in 1D mirror twin boundaries of single-layer MoSe2. Nat. Phys. 12, 751–756 (2016).
Wang, L. et al. Direct Observation of One-Dimensional Peierls-type Charge Density Wave in Twin Boundaries of Monolayer MoTe2. ACS Nano 14, 8299–8306 (2020).
Jolie, W. et al. Tomonaga-Luttinger Liquid in a Box Electrons Confined. Phys. Rev. X. 9, 011055 (2019).
Xia, Y. et al. Charge Density Modulation and the Luttinger Liquid State in MoSe2 Mirror Twin Boundaries. ACS Nano 14, 10716–10722 (2020).
Mielke, A. Exact ground states for the Hubbard model on the Kagome lattice. J. Phys. A: Math. Gen. 25, 4335–4345 (1992).
Kiesel, M. L., Platt, C. & Thomale, R. Unconventional Fermi Surface Instabilities in the Kagome Hubbard Model. Phys. Rev. Lett. 110, 126405 (2013).
Zhang, S. H. et al. Kagome bands disguised in a coloring-triangle lattice. Phys. Rev. B 99, 100404 (2019).
Zhang, J. et al. Single-layer Mo5Te8 - A new polymorph of layered transition-metal chalcogenide. 2D Mater. 8, 015006 (2020).
Dong, L. et al. Charge Density Wave States in 2H-MoTe2 Revealed by Scanning Tunneling Microscopy. Chin. Phys. Lett. 35, 066801 (2018).
Yu, Y. et al. Molecular beam epitaxy growth of atomically ultrathin MoTe2 lateral heterophase homojunctions on graphene substrates. Carbon 115, 526–531 (2017).
Coelho, P. et al. Post-Synthesis Modifications of Two-Dimensional MoSe2 or MoTe2 by Incorporation of Excess Metal Atoms into the Crystal Structure. ACS Nano 12, 3975–3984 (2018).
Jiao, L. et al. Molecular-beam epitaxy of monolayer MoSe2: growth characteristics and domain boundary formation. N. J. Phys. 17, 053023 (2015).
Kim, D. & Liu, F. Realization of flat bands by lattice intercalation in kagome metals. Phys. Rev. B 107, 205130 (2023).
Yu, Y. et al. Phase-controlled growth of one-dimensional Mo6Te6 nanowires and two-dimensional MoTe2 ultrathin films heterostructures. Nano Lett. 18, 675–681 (2018).
Weitering, H. H. et al. Defect-mediated condensation of a charge density wave. Science 285, 2107–2110 (1999).
Horcas, I. et al. WSXM: a software for scanning probe microscopy and a tool for nanotechnology. Rev. Sci. Instrum. 78, 013705 (2007).
Kresse, G. & Furthmuller, J. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Phys. Rev. B 54, 11169–11186 (1996).
Klimeš, J., Bowler, D. R. & Michaelides, A. Van der Waals density functionals applied to solids. Phys. Rev. B 83, 195131 (2011).
Acknowledgements
This project is supported by Strategic Priority Research Program and Key Research Program of Frontier Sciences and Instrument Developing Project (Chinese Academy of Sciences, CAS) [No. XDB30000000 (Z.C. and W.J.), No. QYZDB-SSW-SYS031 (Z.C.), No. YZ201418 (Z.C.)], the National Natural Science Foundation of China (NSFC) [No. 21622304 (Z.C.), 61674045 (Z.C.), 11604063 (R.X.), 11974422 (W.J.), 12104504 (W.J.)], the National Key R&D Program of China [Grant No. 2018YFE0202700 (Z.C.)]. Z. H. Cheng was supported by Distinguished Technical Talents Project and Youth Innovation Promotion Association CAS, the Fundamental Research Funds for the Central Universities and the Research Funds of Renmin University of China [No. 21XNLG27 (Z.C.), No. 22XNKJ30 (W.J.), No. 22XNH095 (H.D.)]. Calculations were performed at the Physics Lab of High-Performance Computing of Renmin University of China, Shanghai Supercomputer Center and Beijing Supercomputing Center.
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Z.C., G.W. and W.J. conceived the research project. L.L., H.D., Y.G. and Z.C. performed the STM experiments and analysis of STM data. R.X., F.P. and F.L. helped in the experiments. J.D., F.C., C.W., Z.L., and W.J. performed the DFT calculations. L.L., J.D., F.C., Z.C. and W.J. wrote the manuscript with inputs from all authors.
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Lei, L., Dai, J., Dong, H. et al. Electronic Janus lattice and kagome-like bands in coloring-triangular MoTe2 monolayers. Nat Commun 14, 6320 (2023). https://doi.org/10.1038/s41467-023-42044-5
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DOI: https://doi.org/10.1038/s41467-023-42044-5
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