Skip to content
See the World Through ScienceA project of ALLATRA
Source: Peer-reviewedNature1 source

Atom-Thin Crystals Now Start Growing Where Engineers Put Them, Not at Random

AI & Technology

Republish this story

Our work is licensed under Creative Commons BY-NC 4.0. You may republish this piece for free — with credit to ALLATRA Media and a link to the original, unedited beyond length trims, and not for commercial use.

Read the full license

Scanning electron micrographs: a grid of patterned growth sites, each holding one triangular crystal of molybdenum disulfide at its center, with micrometer scale bars and a labeled hafnium oxide barrier.
Scanning electron micrographs from the Oct. 7, 2026, paper: a single triangular crystal of molybdenum disulfide grows at the center of each patterned site, ringed by a hafnium oxide barrier (panels d to g).Fig. 1 from Jeongwon Park et al. (2026), "Spatially deterministic nucleation of 2D semiconductors by etching flux", Nature — CC BY 4.0

A team at KAIST and the Daejeon company TDS Innovation has reported a growth process that fixes where a single flake of an atom-thin semiconductor starts forming, putting it at the center of each patterned site instead of letting it appear at a random point. The work was published Oct. 7, 2026, in Nature.

The paper states that existing methods can confine growth to the areas a designer chooses but cannot decide where inside an area an individual crystal begins, which limits how large a single crystal can get and leaves its position unpredictable. The authors write that such precision governs how uniform the resulting layer is and how well the devices built on it perform.

Each growth area is ringed by a barrier of hafnium oxide. Jeongwon Park, Kibum Kang and colleagues report that the barrier gives off oxygen at the growth temperature, that the oxygen etches away crystals trying to form near the pattern edge, and that the only crystal left to grow is the one that started at the geometric center. Across 400 patterned sites they measured a single-crystal yield exceeding 99 percent, single crystals of molybdenum disulfide about 10 micrometers across, and a field-effect mobility, a measure of how easily current moves through a channel, of up to 117 cm² V⁻¹ s⁻¹.

A diagram of a patterned growth region with oxygen spreading inward from the barrier, a reaction-rate plot above it, and X-ray measurements of the barrier material below.
The barrier gives off oxygen at growth temperature, which eats away anything starting near the pattern edge and leaves the center the only place a crystal survives (panels a to c of Fig. 2). Fig. 2 from Jeongwon Park et al. (2026), "Spatially deterministic nucleation of 2D semiconductors by etching flux", Nature — CC BY 4.0

The process also worked on non-crystalline silicon dioxide, not only on crystalline sapphire. A zirconium dioxide barrier brought the growth temperature down to 430 °C, and several transistors were built inside one large crystal. These are laboratory growth runs at the micrometer scale, and the paper does not address production at the scale of a full wafer. The authors describe the approach as a path toward denser integration of atom-thin electronics.

The paper's competing-interests declaration records that Kibum Kang, one of its corresponding authors, is a co-founder and the chief executive of TDS Innovation, and that other co-authors are employees of the company or sit on its board.

Sources

Spot an error?

Spot an error?

Report an error

Spotted a mistake on this page? Tell us what's wrong and our editors will take a look.

What kind of problem?

Only if you'd like us to be able to follow up. We won't use it for anything else.

We correct mistakes openly. Select any text to flag it. Fixes are logged under our Corrections Policy.

Report an error

Reporting on

Atom-Thin Crystals Now Start Growing Where Engineers Put Them, Not at Random

What kind of problem?

Only if you'd like us to be able to follow up. We won't use it for anything else.

We read every report. Corrections are logged publicly.