Brown Researchers Keep Electric and Magnetic Order in 1.6-Nanometer Film

Editorial illustration of a woman materials scientist inspecting a wafer in a nanofabrication laboratory; not a photo of Brown researchers.

November 2, 2026 — Brown University researchers in Providence, Rhode Island, have reported a way to retain both electric and magnetic order in ultrathin bismuth ferrite, even at just four atomic unit cells, approximately 1.6 nanometers. Their October 28 study in Nature Materials advances a potential building block for low-power logic and memory, rather than demonstrating a finished processor.

The obstacle has been the “dead layer”: as multiferroic films shrink, disrupted crystal structure and unwanted electric fields can erase the properties engineers hope to exploit. In its research announcement, Brown explains how the team tackled both mechanisms instead of simply making a thicker film.

Engineering Away the Dead Layer

The researchers grew bismuth ferrite on a dysprosium scandate substrate, using lattice mismatch to compress and stabilize the film. A conductive strontium ruthenate layer screens disruptive electric fields. The combined boundary conditions preserved ferroelectric and magnetic behavior at device-relevant thicknesses, according to atomic-resolution imaging, magnetic measurements and calculations.

Simplified schematic of bismuth ferrite film on strontium ruthenate electrode and dysprosium scandate substrate.
Original explanatory diagram based on Brown University and Nature Materials (2026); not a micrograph and not to physical scale.

Importantly, the experiments also showed signatures of altermagnetism, a magnetic ordering pattern of interest because it may support dense, fast information readout. This is a materials result: the paper does not report a working AI chip, a processor clock rate, or a verified reduction in energy per computation.

What the Thickness Data Really Show

The study examines film thicknesses including 1.6, 3.6 and 50 nanometers. Those numbers describe research samples, not a performance comparison. We use a vertical bar chart rather than a time-series line because these are discrete thickness groups, not measurements changing over time.

Vertical bar chart comparing 1.6, 3.6, and 50 nanometer bismuth ferrite film thicknesses.
Selected BFO sample thicknesses, not chip performance or measured power efficiency. Source: Fratian et al., Nature Materials (2026).

Earlier 2024 work at Switzerland’s Paul Scherrer Institute imaged coupled magnetic and ferroelectric textures in bismuth ferrite. Its picture below illustrates the established physical phenomenon; it is not an image from Brown’s new experiment.

Red-blue ferroelectric domain map in bismuth ferrite from Paul Scherrer Institute 2024 research.
Archival Paul Scherrer Institute (2024) nanoscale magnetic/ferroelectric imaging; background illustration, not Brown’s 2026 data.

Why It Matters—and What Is Missing

For computing, the attraction is nonvolatile switching driven by modest voltage pulses. But progress in post-silicon chip materials and gallium-nitride power devices shows that promising laboratory physics and scalable manufacturing remain separate challenges.

The practical comparison is with devices already shipping or being commercialized. Our reports on ultralow-power microcontrollers, semiconductor process contamination and edge-AI silicon track different pieces of that transition.

Next come device prototypes, repeatable switching and endurance tests, compatibility with semiconductor fabrication, and measured energy-per-operation results. Until those data exist, claims of dramatically more efficient AI chips remain prospects, not demonstrated system-level savings.

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