Liquid metal prints fast transistors express

Original: "High-Mobility Indium Native Oxide Transistors via Liquid-Metal Printing in Air"
arXiv:2604.06656 · 2026-04-08 · CC BY-SA 4.0 · 1 min
A thin film of indium oxide, printed in the open air, conducts electricity almost as well as the best vacuum-deposited samples.

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An ordinary transistor in a phone is made in a vacuum chamber, where atoms are deposited layer by layer. Expensive and slow. But indium oxide can be printed like ink — from a drop of liquid metal that, in air, coats itself with a thin oxide film.

The authors took indium, melted it, and rolled it over a substrate at 250 degrees. The result was a polycrystalline layer only 5 nanometers thick — a thousand times thinner than a human hair. Its grains are large and span the entire thickness, so electrons move almost without obstacles.

A mobility of 125 cm²/V·s is like a sprinter's speed: an electron in such a channel outruns its counterparts in most printed semiconductors.

The transistor built on this film works stably: after 10,000 on-off cycles, its characteristics did not degrade. And if you add a hafnium oxide insulator, the mobility stays high—107 cm²/V·s — while leakage current is minuscule. From such transistors, the team built an inverter, a basic logic element, and it amplifies the signal by a factor of 69.8.

Printing oxide semiconductors from liquid metal is like cooking on a skillet instead of molecular gastronomy: simpler, faster, and almost as tasty. The next step is to shrink the transistors and test them in real circuits.

Original abstract

as written by the authors arXiv:2604.06656

Oxide semiconductors have emerged as common channel materials in transistors and hold promise for next-generation electronics, yet achieving high mobility typically requires costly vacuum-based techniques. Here, ultrathin (5-nm) indium native oxide (InOx) prepared by ambient-air liquid-metal printing (LMP) at low temperature (250 {\deg}C), is applied as semiconducting channel in field-effect transistor (FET). The resulting InOx is found to be polycrystalline with large lateral grains that extend vertically throughout the film thickness. InOx FETs in a transfer length method (TLM) configuration demonstrate a high conductivity mobility (uCON) of 125 cm2 V-1 s-1, with systematic analysis of contact resistance confirming potential for channel length scaling. Integration with atomic-layer-deposited (ALD) gate dielectrics further reveals excellent compatibility, for instance, InOx FET integrated with HfO2 exhibits a high field-effect mobility (uFE) of 107 cm2 V-1 s-1, an on/off current ratio (ION/IOFF) of >107, a subthreshold swing (SS) of 204 mV dec-1, a gate leakage of <10-6 A cm-2, while maintaining stable performance over 104 endurance cycles without degradation. Post-fabrication oxygen-plasma treatment is applied to achieve enhancement-mode operation and a depletion-load inverter is demonstrated, exhibiting a voltage gain of 69.8 V/V. These results demonstrate the great potential of LMP InOx as semiconducting channel in high-performance and power-efficient transistors for next-generation oxide electronics.

An indium oxide film just 5 nanometers thick is transparent to the eye but conducts electricity — which is why such materials are used in touchscreens.

In the series 'Westworld,' robots are covered with thin films that are printed on the spot — similar to this technology, but for electronics.

\mu_{CON} = \frac{L}{R_{ch} \cdot C_{ox} \cdot W}
Charge mobility (mu) is the ratio of channel length L to the product of channel resistance R_ch, insulator capacitance C_ox, and channel width W. The higher the mu, the faster the transistor.
Scientists
Paul DiracEmmy NoetherWolfgang PauliEnrico FermiChien-Shiung WuEugene Wigner
Concepts
high temperature superconductor liquid nitrogen silicon carbide high temperature superconductivity liquid helium gallium arsenide metal insulator transition solid electrolyte titanium oxide silicon wafer thin film superconductivity superconducting wire semiconductor aluminum nitride thin film topological insulators ion channel lithium ion molybdenum disulfide insulator niobium nitride