In plain words

Flaws that appear when a thin layer is laid on a surface or on another layer. Water and dirt trapped underneath gather into small bubbles that push the layer up, and a layer with more length than the surface beneath it folds into wrinkles. Both stretch or bend the layer where they sit and change how it conducts and glows there, so careful stacking keeps them away from the part that is measured.

As the site uses it

Best-quality 2D layers are usually grown at temperatures above what finished circuitry can tolerate, then moved onto the target wafer in a wet transfer process that tears, wrinkles and dirties them.

What 2D materials are good for

Peeling the film off its catalyst and floating it onto another surface introduces tears, wrinkles, polymer residue and trapped bubbles, and it is the single biggest gap between laboratory graphene and industrial graphene.

What is a 2D material?

Going deeper

Left: cross-section of a layer lying on a bottom crystal such as hBN, flat and clean on both sides of a dome in which dots of trapped water and hydrocarbons have gathered; the bulge stretches the layer, and bubbles of any size share much the same shape. Right: cross-section of a layer on a substrate with a narrow ridge, squeezed from both sides – a wrinkle where the layer has more length than the surface, left by transfer or by cooling after growth on copper, which shrinks while graphene does not. a bubble between two layers trapped water and hydrocarbons gather into a bubble clean, flat clean, flat bottom crystal, for example hBN the bulge stretches the layer above it; bubbles of any size share much the same shape a wrinkle a ridge where the layer has more length than the surface squeezed squeezed substrate from transfer, or from cooling after growth: copper shrinks, graphene does not
Trapped contamination gathers into bubbles and leaves clean interface around them; a wrinkle is a fold where a layer has more length than the surface under it. Both strain the layer and change it locally.

Why dirt gathers into bubbles

Two flat crystals pressed together attract each other over their whole area. Water and hydrocarbons trapped between them hold the layers apart, so the attraction squeezes them sideways until they collect in pockets, and the interface in between is left clean to the atom – cross-sections imaged in the electron microscope showed exactly that. , or stacking at a higher temperature as in the , lets the contamination travel further, so it gathers into fewer, larger bubbles or is pushed out of the stack altogether.

Bubbles are easy to find: they show up in images and in dark-field optical microscopy, and good practice is to map them before deciding where the contacts go.

Strain and pressure inside a bubble

The shape of a bubble is a balance between the adhesion pulling the layer down and the stiffness of the layer resisting the bulge. Measured by AFM on graphene, hBN and MoS2, bubbles of every size turned out to have nearly the same shape for a given pair of materials, and the substance trapped in submicron bubbles sits at pressures of tens of megapascals.

The bulge stretches the layer, which shifts its and peaks. In WSe2 such strained spots can trap and emit single ; in graphene the uneven of nanobubbles acts on the electrons like a magnetic field of more than 300 tesla.

Wrinkles

A wrinkle forms where a layer has more length than the surface under it. Transfer leaves them when a film does not lie down evenly, and growth leaves them too: copper shrinks much more than graphene as the foil cools after growth, so the graphene has to buckle. In large-area films wrinkles are one of the flaws that lower , and current that has to cross them meets extra resistance.

For specialists

Blisters of trapped adsorbates – mainly hydrocarbons and water – between or stacked layers, from nanometres to micrometres across, and ridges where compressive strain from transfer or thermal-expansion mismatch is relieved out of plane. adhesion squeezes contamination into bubbles, leaving atomically clean interfaces between them, and the bubbles take a universal shape set by adhesion and in-plane stiffness. Both strain the layer locally, shifting band edges, Raman modes and emission, and both scatter carriers.

Where this comes from

  1. Strain-induced pseudo-magnetic fields greater than 300 tesla in graphene nanobubbles Levy et al. · Science 329, 544 (2010)
  2. Cross-sectional imaging of individual layers and buried interfaces of graphene-based heterostructures and superlattices Haigh et al. · Nature Materials 11, 764 (2012)
  3. Structure and electronic transport in graphene wrinkles Zhu et al. · Nano Letters 12, 3431 (2012)
  4. Universal shape and pressure inside bubbles appearing in van der Waals heterostructures Khestanova et al. · Nature Communications 7, 12587 (2016)