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Van der Waals heterostructures

A. K. Geim, I. V. Grigorieva
Nature·2013·Materials science·10,527 citations
8 min read

Read the full paper at DOI or on arxiv

TL;DR

The review argues that vdW heterostructures enable atomic-scale “Lego-like” assembly of 2D crystals, turning interfaces into a tunable design parameter.

Briefing

This Nature article by A. K. Geim and I. V. Grigorieva is a forward-looking review of “van der Waals (vdW) heterostructures”: artificial materials assembled by stacking atomically thin two-dimensional (2D) crystals in a chosen sequence with one-atomic-plane precision. The central research question is not a single hypothesis tested experimentally, but rather: why vdW heterostructures matter, how they work in practice, what materials are realistically available for assembly, and what directions are most promising for future fundamental physics and applications.

The importance of the topic is framed by the trajectory of graphene research. Graphene has matured from a discovery phase into a vast application-driven field (the authors note on the order of 10,000 papers per year), and they argue that “simple graphene” has passed its peak. At the same time, the fundamental physics of graphene is still not exhausted, and device quality continues to improve. However, the authors emphasize that progress is now increasingly driven by using graphene as a platform and by expanding to other 2D crystals such as hexagonal boron nitride (hBN) and transition-metal dichalcogenides (e.g., MoS a). The review’s broader context is therefore the shift from studying a single material to engineering designer “layer-by-layer” systems where the interface itself becomes a tunable component.

Methodologically, the paper is a synthesis of the emerging experimental literature rather than a new study with a defined sample size. The “method” is the conceptual and practical workflow of vdW heterostructure fabrication: (i) isolate micrometre-sized exfoliated 2D flakes (often via the Scotch tape method), (ii) transfer them face-down onto a target using optical alignment and micromanipulators, (iii) remove the supporting polymer/film, and (iv) repeat until the desired stack is built. For device fabrication, the authors describe subsequent lithography and plasma etching into Hall-bar geometries, plus metal contact evaporation. They also discuss an alternative “vertical” device route where thin hBN, MoS a, or WS a layers act as tunnel barriers between graphene electrodes.

A key practical theme is that vdW heterostructures work “exceptionally well” because interfaces can be made atomically sharp and clean despite ubiquitous contamination on exposed 2D surfaces. The authors explain this using the physics of vdW adhesion: when two layers are brought into contact, vdW forces can squeeze out trapped contaminants or expel them into micrometre-scale “bubbles,” yielding interfaces that are clean and sharp on the scale relevant for electronic transport. They cite cross-sectional imaging work showing clean buried interfaces and note that contamination can be effectively removed at interfaces.

The review’s key findings are presented as concrete empirical benchmarks and device demonstrations from the literature. For materials quality and device performance, the authors highlight that encapsulated graphene on hBN can reach mobilities on the order of 100,000 cmVs, and up to about 500,000 cmVs at low temperature. They also cite room-temperature ballistic transport in encapsulated graphene, including negative bend resistance and magnetic focusing signatures. For quantum capacitance, they mention that capacitors larger than 100 m can show quantum oscillations at magnetic fields as low as about 0.2 T.

For heterostructure functionality beyond encapsulation, the authors summarize several “evolutionary steps.” First, hBN’s role as a high-quality substrate for graphene is credited as a major enabling advance. Second, encapsulation with thin hBN is described as stabilizing device quality against ambient degradation. Third, vertical tunnelling devices are described as a major step: by using few-layer hBN (or other 2D crystals) as tunnel barriers, one can realize field-effect tunnelling transistors where the tunnel current is controlled by gate-tuned changes in graphene’s Fermi energy. The authors report on-off switching ratios exceeding at room temperature for these vertical tunnelling devices.

For more complex stacks, the review points to a graphene–hBN superlattice consisting of six alternating bilayers (the largest number of 2D crystals reported at the time). It also discusses double-layer graphene devices where two graphene sheets are separated by as little as three hBN layers, corresponding to a separation of roughly 1 nm. The authors emphasize that even at this separation, tunnelling is suppressed while interlayer Coulomb interactions remain strong, enabling exploration of many-body states. They report that the measurements in zero magnetic field have not yet shown evidence of interlayer excitonic superfluidity, despite the expectation that the Coulomb energy scale could be large (they state it can exceed 0.1 eV). They also note that the most promising route for coherent states may be in quantizing magnetic fields, which at the time had not been fully explored in this context.

A particularly important “result” for the review is the role of crystallographic alignment and moir patterns. The authors cite graphene on hBN superlattices where alignment accuracy better than about 1 can be achieved. In these systems, moir potentials reconstruct the electronic spectrum, producing additional Dirac cones at high carrier densities. They state that the Hall effect can change sign and that the new Dirac cones show their own Landau levels. The authors interpret these strong spectral effects as evidence that interfacial contamination is negligible and that vdW heterostructures can be used for band-structure engineering.

The review also provides a “reality check” on what 2D crystals can actually survive and be used. The authors argue that many theoretically imaginable 2D materials are unlikely to be stable when exfoliated because melting temperature decreases with decreasing thickness and because monolayers have no bulk to protect them from surface reactions. They give specific stability examples: MoS begins oxidizing in moist air around 85C, and they note that graphene would not survive if room temperatures were doubled to around 300C. They also discuss that many materials stable in bulk corrode or decompose when thinned (e.g., GaSe, TaS, BiSe). They highlight that contamination is trapped between layers unless it can be cleared; vdW adhesion and annealing can mitigate this.

Limitations are acknowledged implicitly through the review’s emphasis on practical constraints: (i) the available library of stable 2D crystals is limited, (ii) fabrication requires months to master even though the conceptual stacking is simple, (iii) scalable manufacturing is not yet solved, and (iv) many speculative “big dreams” may fail because the field is still early and parameter space is vast. The authors also note that knowledge about oxide and hydroxide monolayers is limited largely to microscopy observations, with few electrical measurements.

Finally, the review discusses practical implications. Who should care includes condensed-matter physicists interested in many-body phenomena (e.g., Wigner crystallization, excitonic superfluidity, itinerant magnetism), device engineers seeking new transistor and tunnelling architectures, and materials scientists focused on scalable production. The authors argue that vdW heterostructures can accelerate the application roadmap already associated with graphene by enabling new device architectures (encapsulation, vertical tunnelling, superlattices, and proximity effects). For industrial scale, they discuss several approaches—vdW epitaxy, Langmuir–Blodgett-like layer deposition, and self-assembly from suspensions—but conclude that the most feasible route at the time is to grow mono- and few-layer sheets on catalytic substrates, then isolate and transfer them to build stacks. They predict a “snowball effect” as more groups adopt the technology and explore the combinatorial parameter space of materials, sequences, and alignments.

Overall, the paper’s contribution is to consolidate the field’s enabling principles (materials stability, contamination control, and atomic-scale assembly), to report key performance benchmarks from representative experiments, and to chart a roadmap for future physics and scalable engineering of vdW heterostructures.

Cornell Notes

Geim and Grigorieva review how stacking atomically thin 2D crystals via van der Waals forces enables “designer” heterostructures with clean, atomically sharp interfaces. They synthesize fabrication methods, realistic constraints on which 2D materials survive, and key device/physics demonstrations (encapsulated graphene, vertical tunnelling transistors, moir superlattices, and double-layer graphene many-body platforms).

What is the main idea behind van der Waals heterostructures?

Assemble atomically thin 2D crystals in a chosen sequence, using strong in-plane covalent bonds for stability and relatively weak vdW-like forces to hold the stack together with one-atomic-plane precision.

Why do the authors argue vdW heterostructures are scientifically important now?

Because graphene’s “simple” phase is maturing, and the field is shifting toward using graphene as a platform while expanding to other 2D crystals; stacking enables new interface-driven phenomena and device architectures.

What practical fabrication workflow do the authors describe?

Isolate micrometre-sized 2D flakes, transfer them face-down onto a target under optical microscopy using micromanipulators, remove the supporting polymer/film, repeat for each layer, then pattern devices (e.g., Hall bars) and add contacts.

What evidence do the authors cite that interfaces can be clean and atomically sharp?

They report that vdW adhesion can squeeze out trapped contaminants or push them into micrometre-scale bubbles, enabling interfaces that are clean and sharp; strong moir-driven spectral reconstruction in graphene/hBN is presented as additional evidence that contamination is negligible.

What performance benchmarks are highlighted for encapsulated graphene?

Encapsulated graphene mobilities are cited as 100,000 cmVs and up to about 500,000 cmVs at low temperature, with ballistic effects persisting up to room temperature.

What is the reported room-temperature switching performance of vertical tunnelling devices?

Field-effect tunnelling transistors based on vertical graphene heterostructures are described as having on-off switching ratios greater than at room temperature.

What is the significance of double-layer graphene devices?

They separate two graphene sheets by as little as three hBN layers (about 1 nm), suppressing tunnelling while keeping strong interlayer Coulomb interactions, enabling tests of many-body states such as interlayer excitonic superfluidity.

What do the authors report about excitonic superfluidity in double-layer graphene?

Measurements in zero magnetic field show no sign of superfluidity so far, though quantizing magnetic fields are suggested as the most promising regime for coherent states.

How does crystallographic alignment affect electronic structure in graphene/hBN heterostructures?

With alignment accuracy better than about 1, moir potentials reconstruct the spectrum, producing additional Dirac cones; the Hall effect can change sign and the new Dirac cones show their own Landau levels.

What do the authors conclude about scalability for industrial production?

They discuss multiple scalable routes (vdW epitaxy, Langmuir–Blodgett-like deposition, self-assembly from suspensions) but argue the most feasible approach is to grow mono-/few-layer sheets on catalytic substrates and then isolate and transfer them to build stacks.

Review Questions

  1. What physical mechanism allows vdW heterostructures to achieve clean, sharp interfaces despite contamination on exposed 2D surfaces?

  2. Which experimental benchmarks in the review are used to justify that encapsulated graphene and vdW stacks reach high electronic quality?

  3. How do moir patterns arising from alignment modify graphene/hBN electronic spectra, and why is this used as evidence against significant interfacial contamination?

  4. Why do double-layer graphene devices suppress tunnelling yet still maintain strong interlayer interactions, and what many-body phenomena are targeted?

  5. What constraints limit the “2D library” of materials suitable for vdW assembly, and how do the authors propose expanding it?

Key Points

  1. 1

    The review argues that vdW heterostructures enable atomic-scale “Lego-like” assembly of 2D crystals, turning interfaces into a tunable design parameter.

  2. 2

    A major enabling factor is that vdW contact can squeeze out trapped contamination, producing clean, atomically sharp interfaces (supported by imaging and by strong moir-driven electronic reconstruction).

  3. 3

    Encapsulated graphene on hBN achieves very high mobility (about cmVs, up to at low temperature) and ballistic effects persisting to room temperature.

  4. 4

    Vertical graphene tunnelling heterostructures using thin 2D barriers enable field-effect tunnelling transistors with room-temperature on-off switching ratios exceeding .

  5. 5

    Double-layer graphene devices use ~1 nm separation (three hBN layers) to suppress tunnelling while keeping strong interlayer Coulomb coupling; no zero-field excitonic superfluidity is observed yet.

  6. 6

    Crystallographic alignment (better than about 1) in graphene/hBN creates moir superlattices that reconstruct the band structure, including additional Dirac cones and Hall-sign changes.

  7. 7

    The practical limitation is materials stability: many monolayers corrode or decompose in air, so the usable 2D library is smaller than theoretical possibilities.

  8. 8

    Scalability remains a challenge; the authors view growth on catalytic substrates followed by transfer as the most feasible industrial path at the time of writing.

Highlights

“Strong covalent bonds provide in-plane stability of 2D crystals whereas relatively weak, van der Waals-like forces are sufficient to keep the stack together.”
“The reason for the clean interfaces is the vdW forces that attract adjacent crystals and effectively squeeze out trapped contaminants or force them into micrometre-sized ‘bubbles’.”
Encapsulated graphene mobilities are cited as “ cmVs” and “up to 500,000 cmVs at low T.”
Vertical field-effect tunnelling transistors are described as having “on-off switching ratio > at room T.”
In graphene/hBN superlattices, “the Hall effect changes its sign” and “new Dirac cones exhibit their own sets of Landau levels.”

Topics

  • Condensed matter physics
  • Two-dimensional materials
  • Materials interfaces
  • Quantum transport
  • Moir superlattices
  • Many-body physics
  • Tunnelling and field-effect devices
  • Semiconductor heterostructures
  • Materials synthesis and exfoliation
  • Scalable nanomanufacturing

Mentioned

  • Scotch tape technique
  • Plasma etching
  • Langmuir–Blodgett deposition
  • Langmuir-Blodgett (LB)
  • Micromanipulators
  • Cleanroom fabrication
  • Transmission electron microscopy (TEM)
  • Scanning probe microscopy
  • Hall bar devices
  • Molecular beam epitaxy (MBE)
  • A. K. Geim
  • I. V. Grigorieva
  • K. S. Novoselov
  • V. I. Falko
  • L. Colombo
  • P. R. Gellert
  • M. G. Schwab
  • K. Kim
  • C. R. Dean
  • A. S. Mayorov
  • A. H. MacDonald
  • J. Jarillo-Herrero
  • K. Watanabe
  • T. Taniguchi
  • B. Radisavljevic
  • A. Radenovic
  • A. Britnell
  • L. Britnell
  • R. V. Gorbachev
  • T. Georgiou
  • S. J. Haigh
  • L. A. Ponomarenko
  • R. V. Gorbachev
  • G. L. Yu
  • R. R. Nair
  • R. J. Young
  • K. S. Novoselov
  • T. F. Heinz
  • B. J. van Wees
  • vdW - van der Waals
  • 2D - two-dimensional
  • hBN - hexagonal boron nitride
  • MoS2 - molybdenum disulfide
  • WS2 - tungsten disulfide
  • WSe2 - tungsten diselenide
  • BSCCO - bismuth strontium calcium copper oxide
  • TC - critical temperature
  • FET - field-effect transistor
  • MBE - molecular beam epitaxy
  • STM - scanning tunneling microscopy
  • TEM - transmission electron microscopy
  • μ - carrier mobility
  • B - magnetic field
  • eV - electronvolt
  • T - temperature
  • Dirac cone - linear dispersion feature in graphene-like band structures