What they are and why they matter
How a one-atom-thick crystal is made, what it is already used for, and which promises are still hype.
“Is graphene actually in anything I can buy?”
Start with the basicsEach dot is a carbon atom. The large pattern is the moiré; its period follows λ = a / 2 sin(θ/2).
News and explainers on two-dimensional materials
Stack two layers of graphene, rotate one by just over a degree, and near absolute zero the pair becomes a superconductor. Materials this thin behave nothing like their bulk crystals. Flatland follows what they are, what they are good for, and what is still hype.
The same material reads differently to a curious reader, a theoretician, a crystal grower and a process engineer. Pick the depth that fits; the lens in the header remembers it.
How a one-atom-thick crystal is made, what it is already used for, and which promises are still hype.
“Is graphene actually in anything I can buy?”
Start with the basicsMoiré correlations, zero-field fractional states, excitons and 2D magnetism – and the pitfalls of computing them.
“Why does my GW gap drift with vacuum size?”
Open the theory trackConditions that work, the signatures that diagnose what you made, and the ways experiments go wrong without anyone noticing.
“Is this a Janus layer or just an alloy?”
Open the experiment trackReadiness levels with reasons, integration constraints, supply risks, and who is building what.
“What actually blocks 2D transistors at 300 mm?”
Open the engineering trackPicked for everyonePicked for theoreticiansPicked for experimentalistsPicked for engineers · updated 5 Oct 2026
Collected from 137 journal, preprint and news feeds. The lens in the header changes what comes first. Preprints are marked because they have not been peer reviewed yet.
Researchers at Dongguk University in South Korea have developed a battery-free, flexible graphene transistor that mimics biological synapses and can recognize human activity without any external power source. A self-powered graphene-channel transistor, driven entirely by triboelectric nanogenerators, mimics biological…
Heat flow in the Chern Insulator states of the Hofstadter butterfly is obtained in a graphene/hBN moiré for the first time. [Phys. Rev. Lett. 137, 146603] Published Tue Sep 29, 2026
Twistronics has become a new alchemy of materials. By choosing atomically thin layers, stacking them and changing their relative angle, researchers can create electronic behavior absent from the original ingredients. Twisted graphene and transition metal dichalcogenides have already yielded superconductivity and…
Atomically aligned 1H bilayer MoS2 exhibits a direct band gap, enhanced excitonic emission and stronger valley polarization, establishing its potential for advanced optoelectronic and valleytronic applications.
A drop of coffee on a tabletop often leaves a dark ring behind. This everyday mark is a reminder that a drying droplet is not passive: As water evaporates, it can transport the particles suspended inside it toward the edge. Scientists call this the coffee-ring effect. For inkjet printing and surface coatings, however…
A central goal of the emerging field of materials QED is to harness subwavelength electromagnetic confinement in engineered cavities to tailor light-matter interactions. Here, we demonstrate that van der Waals multilayer cavities composed of stacked graphene and hexagonal boron nitride (hBN) provide unprecedented…
We theoretically investigate the optical response of the WSe2 monolayer vertically stacked on twisted bilayer graphene (tBG) under electrostatic doping. In this heterostructure, the doped moiré superlattice of tBG generates a spatially modulated electrostatic potential that couples to the electron and hole constituents…
We theoretically investigate the optical response of the WSe2 monolayer vertically stacked on twisted bilayer graphene (tBG) under electrostatic doping. In this heterostructure, the doped moiré superlattice of tBG generates a spatially modulated electrostatic potential that couples to the electron and hole constituents…
Most proposals for Z3 parafermions in fractional quantum Hall-superconductor structures used the spin-unpolarized ν= 2/3 Halperin (1,1,2) state. The fractional quantum anomalous Hall (FQAH) states of twisted MoTe2 and rhombohedral graphene are believed to be spin- and valley-polarized Jain states, with the same…
Discovering the quantum anomalous Hall (QAH) effect in two-dimensional magnets is a central goal of topological condensed matter physics, yet candidate materials combining a sizable gap with a well-defined Chern number remain scarce. We report a new material platform that realizes emergent magnetism and nontrivial band…
Air-sensitive 2D materials present fundamental challenges for device integration. Encapsulation is required to preserve intrinsic properties, yet conventional strategies require complicated fabrication workflows and fail with thicker flakes. We demonstrate that electron-beam (e-beam) evaporated aluminum oxide (AlOx)…
Spectrally isolated, electrically driven emission from localized states in two-dimensional semiconductors remains challenging in scalable planar devices. Here, we report narrow-line-width alternating-current electroluminescence (ACEL) from localized states in monolayer WSe2 using a lithographically defined sub-5 nm…
Transition metal ditellurides exhibit structural and electronic properties distinct from their selenide and sulfide counterparts, including the stabilization of multiple charge density wave (CDW) phases. Within the niobium compound family, notable differences in structure are also observed: bulk NbTe2 crystallizes in…
We theoretically investigate the optical response of the WSe2 monolayer vertically stacked on twisted bilayer graphene (tBG) under electrostatic doping. In this heterostructure, the doped moiré superlattice of tBG generates a spatially modulated electrostatic potential that couples to the electron and hole constituents…
We numerically study exciton-photon coupling in a hybrid structure composed of a period-doubled Si3N4 photonic crystal slab and an hBN-encapsulated MoSe2 monolayer. Period doubling folds quasi-guided modes into the light cone and produces spectrally separated photonic branches whose radiative character is controlled by…
Hexagonal boron nitride (hBN) is a van der Waals material with excellent insulating properties that make it well-suited as a gate dielectric in 2D electronic devices. In recent years, the discovery of an ever-increasing list of properties has led to a much broader range of potential applications, including quantum…
Researchers at Dongguk University in South Korea have developed a battery-free, flexible graphene transistor that mimics biological synapses and can recognize human activity without any external power source. A self-powered graphene-channel transistor, driven entirely by triboelectric nanogenerators, mimics biological…
We investigate the nanoscale mechanisms determining in-plane lattice thermal conductivity (LTC) of pristine and W-doped MX –M X transition metal dichalcogenide heterobilayers from first principles, using the exact solution of the linearised Boltzmann transport equation in both phonon and relaxon bases. For the W-doped…
Photocatalytic nitrate reduction can couple nitrate removal with ammonia recovery. Successive hydrogenation steps require a local supply of proton equivalents, but making water-derived hydrogen available at nitrate-reduction sites remains difficult. Here, CuCo-LDH supported on anatase TiO2 nanosheets (CuCo-LDH@TNS) is…
Two-dimensional materials are promising candidates for electronic applications beyond the operating limits of conventional semiconductor technologies. Within this class, transition-metal dichalcogenides offer attractive properties for field-effect transistor operation, with tungsten disulphide (WS2) emerging as a…
The next meetingsMeetings for theoreticiansMeetings for experimentalistsMeetings for engineers · as of 5 Oct 2026
Next deadline: 2027 MRS Spring Meeting & Exhibit, abstracts close 14 Oct 2026. The meetings are chosen by hand, never scraped from listing sites.
Abstract submission closed; registration open
Breaking-news abstracts are being accepted; the deadline is on the organiser’s site
Paper and late-news submissions closed; registration open
Abstract submission closed; registration open
Breaking-news abstracts are being accepted; the deadline is on the organiser’s site
The call for abstracts opens in early autumn
Abstract submission closed; registration open
Breaking-news abstracts are being accepted; the deadline is on the organiser’s site
Paper and late-news submissions closed; registration open
Abstract submission closed; registration open
Breaking-news abstracts are being accepted; the deadline is on the organiser’s site
Paper and late-news submissions closed; registration open
Pull a single layer out of a stack and it stops behaving like the block it came from. 8 reasons, explained without equations.
The spacing between layers in graphite
Sheets of graphene needed to match the thickness of one sheet of paper
The fraction of visible light absorbed by a single layer of graphene
The measured breaking strength of defect-free graphene
74 families in 12 groups. Not everything called a 2D material is two-dimensional in the same way, so each one is marked by what kind of sheet it really is.
Graphene and its relatives.
Hexagonal boron nitride, the flat insulator most 2D devices are built on, and other layered nitrides.
A layer of metal atoms sandwiched between two layers of sulfur, selenium or tellurium.
Layered sulfides, selenides and tellurides beyond the dichalcogenides.
Layered compounds of metals, semimetals and pnictogens that cleave into thin flakes.
Single-element sheets beyond carbon.
Metallic carbides and nitrides made by etching one element out of a layered ceramic.
Crystals that stay magnetic down to one or a few atomic layers.
Layers built from two kinds of anion.
Oxide and hydroxide nanosheets, including clays and catalysts.
Sheets of metal halide, bare or separated by layers of organic molecules.
Porous sheets assembled from organic molecules, with or without metal atoms.
18 application areas, sorted by how close they are to something you can buy. Most of what ships today is additives and films, not devices built on a single atomic layer.
The one place 2D materials are already sold by the tonne
Moving heat sideways out of a device with no room for a fan
The first commercial devices where the 2D material really is the active part
A useful additive, not the battery breakthrough that keeps being announced
Storing much less energy than a battery, but delivering it in seconds
Blocking radio noise with something thinner and lighter than metal foil
Slowing rust, when the coating is formulated correctly
Seeing wavelengths that silicon simply cannot see
An electrode that talks to nerve cells without being made of metal
A sieve with holes the size of a single molecule
Circuits that bend, because a layer this thin barely strains when it does
The application graphene was supposed to own, and does not
Cheap catalysts in place of platinum; refineries have used MoS2 for decades
A supporting layer in someone else’s solar cell
The reason chipmakers care, and the slowest thing on this list
Making light one particle at a time, from a defect in a crystal
Memory that computes, built on components that behave like synapses
Beautiful physics, and no product yet
After two decades, the score is clear if you look at what people can buy. 2D materials ship today as additives and films: graphene in composites, coatings, tyres and concrete, graphite-family heat spreaders in phones, conductive additives in battery electrodes, and a few electronic devices, most convincingly graphene magnetic sensors. What did not happen is the version that got the headlines. There is no graphene battery that stores more charge, no mainstream graphene touchscreen, no graphene processor, and graphene has been called a wonder material for twenty years while remaining absent from your laptop. The reasons are consistent across every application: making a perfect small flake is easy and making a merely adequate large one is not, contacting something one atom thick is hard, and incumbent materials are cheap and keep improving.
The credible case for the next decade is narrower and more interesting than the original pitch: 2D semiconductors as a channel material in advanced chips somewhere in the 2030s, because the semiconductor industry has no obvious alternative when silicon stops thinning; niche sensors and medical devices where being all-surface is decisive; and continued unglamorous growth in composites and thermal films. The strongest thing that can be said in the field’s favour is that the industrial research is now being done by chipmakers rather than by enthusiasts, which is usually the sign that a material has stopped being a story and started being an engineering problem. Whether that ends in products is not yet decided, and anyone who tells you otherwise is selling something.
In 1884 the schoolmaster Edwin A. Abbott published Flatland: A Romance of Many Dimensions, a satire narrated by a square who lives in a world of only two dimensions and cannot imagine a third.
When Konstantin Novoselov shared the 2010 Nobel Prize in Physics with Andre Geim for their experiments on graphene, he borrowed that book for the title of his Nobel lecture: Graphene: Materials in the Flatland. Graphene, he wrote, is a two-dimensional object much like Abbott’s world – and just as the story is a romance of many dimensions, graphene is “much more than just a flat crystal”.
This site takes its name from that lecture. The materials it follows are flat; what they do is not.
That prize, and the other Nobel Prizes behind 2D materials
K. S. Novoselov, “Nobel Lecture: Graphene: Materials in the Flatland”, Reviews of Modern Physics 83, 837 (2011)