Twist angle θ1.10°
Moiré period λ12.8 nm
Magic angle: nearly flat bands

Each 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

Two sheets of carbon. Twist one by 1.1°.

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.

Four ways in

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.

Everyone

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 basics
Theoreticians

Frontiers and computational traps

Moiré 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 track
Experimentalists

Growth, transfer and characterisation

Conditions 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 track
Engineers

Readiness and manufacturing

Readiness levels with reasons, integration constraints, supply risks, and who is building what.

“What actually blocks 2D transistors at 300 mm?”

Open the engineering track

Latest

Picked 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 Preprints are marked because they have not been peer reviewed yet.

News Graphene-Info

Self-powered graphene transistor mimics synapses for wearable sensing

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…

EveryoneEngineeringGraphene
Journal Physical Review Letters

Quantized Heat Flow in the Hofstadter Butterfly

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

EveryoneGraphenehBN
News Phys.org

New catalogs map the quantum possibilities of atomically thin materials

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…

EveryoneTheoryGraphene
Preprintnot yet peer reviewed arXiv

Quantum materials QED with van der Waals crystals

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…

Preprintnot yet peer reviewed arXiv

Electrostatic Doping of Moiré Superlattices Controls the Optical Fingerprint of a WSe_2 /Twisted Bilayer Graphene heterostructure

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…

Preprintnot yet peer reviewed arXiv

Electrostatic Doping of Moiré Superlattices Controls the Optical Fingerprint of a WSe_2 /Twisted Bilayer Graphene heterostructure

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…

Preprintnot yet peer reviewed arXiv

Parafermions in fractional Chern insulator-superconductor heterostructures: the role of spin polarization

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…

Preprintnot yet peer reviewed arXiv

Large-gap quantum anomalous Hall insulator in two-dimensional pentagonal TiN8 monolayer

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…

Theory
Preprintnot yet peer reviewed arXiv

Electrostatic Doping of Moiré Superlattices Controls the Optical Fingerprint of a WSe_2 /Twisted Bilayer Graphene heterostructure

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…

Preprintnot yet peer reviewed arXiv

Engineering photonic crystal slab modes for strong exciton-photon coupling and polariton dispersion control

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…

ExperimentMoSe₂hBN
Journal Chemistry of Materials

Low-Temperature Synthesis of Large-Area Hexagonal Boron Nitride Films on Diverse Substrates by Plasma Afterglow Deposition

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…

ExperimentEngineeringhBN
News Graphene-Info

Self-powered graphene transistor mimics synapses for wearable sensing

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…

EveryoneEngineeringGraphene
Preprintnot yet peer reviewed arXiv

Multi-Branch Transport in a Back-gated WS2 Transistor at Deep-Cryogenic Temperature

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…

TheoryEngineeringWS₂

All news

Coming up

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.

Sydney, Australia

RPGR 2026

Abstract submission closed; registration open

Specialist meetingTheoryExperimentEngineering
Boston, USA

2026 MRS Fall Meeting & Exhibit

Breaking-news abstracts are being accepted; the deadline is on the organiser’s site

Society meetingTheoryExperimentEngineering
San Francisco, USA

IEDM 2026

Paper and late-news submissions closed; registration open

Devices and circuitsEngineeringExperiment
Sydney, Australia

RPGR 2026

Abstract submission closed; registration open

Specialist meetingTheoryExperimentEngineering
Boston, USA

2026 MRS Fall Meeting & Exhibit

Breaking-news abstracts are being accepted; the deadline is on the organiser’s site

Society meetingTheoryExperimentEngineering
Kirchberg in Tirol, Austria

IWEPNM 2027

The call for abstracts opens in early autumn

SchoolTheoryExperiment
Sydney, Australia

RPGR 2026

Abstract submission closed; registration open

Specialist meetingTheoryExperimentEngineering
Boston, USA

2026 MRS Fall Meeting & Exhibit

Breaking-news abstracts are being accepted; the deadline is on the organiser’s site

Society meetingTheoryExperimentEngineering
San Francisco, USA

IEDM 2026

Paper and late-news submissions closed; registration open

Devices and circuitsEngineeringExperiment
Sydney, Australia

RPGR 2026

Abstract submission closed; registration open

Specialist meetingTheoryExperimentEngineering
Boston, USA

2026 MRS Fall Meeting & Exhibit

Breaking-news abstracts are being accepted; the deadline is on the organiser’s site

Society meetingTheoryExperimentEngineering
San Francisco, USA

IEDM 2026

Paper and late-news submissions closed; registration open

Devices and circuitsEngineeringExperiment

All conferences

Why thin changes everything

Pull a single layer out of a stack and it stops behaving like the block it came from. 8 reasons, explained without equations.

  1. Squeeze an electron and you change its energy
  2. There is no inside – every atom is a surface atom
  3. Nothing is left hanging, so anything stacks on anything
  4. The material suddenly switches on the light
  5. Extremely strong, and yet you can roll it up
  6. Electrons stop hiding from each other
  7. Three knobs that do not exist in a bulk crystal
  8. In graphene, electrons behave as if they weigh nothing
0.335 nanometres

The spacing between layers in graphite

About 300,000

Sheets of graphene needed to match the thickness of one sheet of paper

2.3 percent

The fraction of visible light absorbed by a single layer of graphene

130 gigapascals

The measured breaking strength of defect-free graphene

Read the basics

The families

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.

  • van der Waals crystal Peels off a layered crystal, one sheet at a time · 58
  • nanosheet Made by chemistry or cut from a solid, not peeled as a clean crystal layer · 12
  • exists only on a substrate Only stable on the surface it was grown on · 3
  • an interface, not a sheet A conducting layer where two crystals meet · 1
13 families

Transition metal dichalcogenides

A layer of metal atoms sandwiched between two layers of sulfur, selenium or tellurium.

13 families

Other layered chalcogenides

Layered sulfides, selenides and tellurides beyond the dichalcogenides.

1 family

MXenes

Metallic carbides and nitrides made by etching one element out of a layered ceramic.

11 families

2D magnets

Crystals that stay magnetic down to one or a few atomic layers.

Browse the catalogue  ·  Compare materials side by side

Where it is real, and where it is not yet

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.

Shipping now

5 areas

In 2–5 years

3 areas

5–15 years away

8 areas

Speculative

2 areas

All applications

Two decades after the sticky tape

The verdict so far

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.

About the name

Why Flatland

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)