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Dual-mode ferroelectric transistors for high-performance generative-adversarial-network-based imaging

Abstract

Artificial intelligence has the capacity to accelerate the interpretation of medical images and support diagnostic decision-making. Delivering these benefits directly within clinical imaging systems, however, requires compact computing hardware capable of executing both generative and discriminative operations with low latency and high energy efficiency. Generative adversarial networks, which combine image synthesis with classification, offer particular promise for improving diagnostic accuracy and augmenting limited datasets, but their implementation in hardware remains challenging owing to competing requirements for rapid weight updates and long-term retention stability. Here we report a reconfigurable neuromorphic platform based on ferroelectric field-effect transistors that enables dual-mode operation via dynamic switching between ferroelectric polarization and charge-trapping mechanisms. This architecture supports both high-speed, energy-efficient synaptic programming and robust non-volatile retention within the same device. Implemented in a 6 × 6 analogue crossbar, the system performs convolution and deconvolution operations representative of generative-adversarial-network workflows, enabling realistic synthesis of mammographic lesions. This approach establishes a compact hardware foundation for embedded diagnostic intelligence in next-generation imaging instruments.

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Fig. 1: Dual-mode FeFETs for GAN hardware configuration.
Fig. 2: Device performance of dual-mode FeFETs.
Fig. 3: Crossbar array modulation.
Fig. 4: Hardware implementation of GAN-based operation.
Fig. 5: Architecture and performance evaluation of GAN for breast lesion detection.

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Data availability

The data that support the plots within this article and other findings of this study are available from the corresponding authors upon reasonable request.

Code availability

All codes are available from the corresponding authors upon reasonable request.

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Acknowledgements

This work is supported by the National Research Foundation (NRF), Prime Minister’s Office, Singapore, under its Competitive Research Program (NRF-CRP24-2020-0002, K.-W.A., NRF-F-CRP-2024-0006, K.-W.A.). L.-J.L thanks the NRF for support (NRF-P2025-002, L.-J.L.). L.-J.L. thanks Nexstrom Pte Ltd, Singapore for MoS2 films.

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Authors and Affiliations

Authors

Contributions

This project was supervised and directed by K.-W.A. and L.-J.L. L.L. and W.M. designed the experiments. C.L. and Y.W. synthesized the MoS2 films. L.L. and H.Z. conducted the device fabrication and electrical measurements. H.Z. conducted high-resolution transmission electron microscopy image analysis. J.W., W.Z. and X.F. contributed to the circuit-level simulations. L.L. and H.X. contributed to the simulation of GAN. C.L., H.Z., J.W., W.Z., J.H., J.G., Y.W. and X.F. contributed to discussion and data analysis. L.L., W.M., L.-J.L. and K.-W.A. wrote the paper. All authors discussed the results and approved the final version of the paper.

Corresponding authors

Correspondence to Wanqing Meng, Lain-Jong Li or Kah-Wee Ang.

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Nature Sensors thanks Yann-Wen Lan and the other, anonymous, reviewer(s) for their contribution to the peer review of this work.

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Extended data

Extended Data Fig. 1 Area ratio dependent on pulse ID-VG behavior.

The area ratio (AR) is defined as the ferroelectric-to-dielectric area proportion. Pulse ID-VG curves measured from representative devices across a sweep width range from 50 µs to 100 ms for area ratios of: a, AR = 0.4; b, AR = 0.3; c, AR = 0.1; d, AR = 0.06; e, AR = 0.04; f, AR = 0.03.

Extended Data Fig. 2 Cycle-to-cycle transfer characteristics for different area ratios.

Dual-sweep DC measurements over 50 cycles at VD = 100 mV with area ratios of: a, AR = 0.4; b, AR = 0.3; c, AR = 0.1; d, AR = 0.06; e, AR = 0.04; f, AR = 0.03. A total of 50 dual-sweep cycles from representative devices is shown, where the light-blue curves represent individual cycles and the dark-blue line indicates one representative cycle.

Extended Data Fig. 3 Benchmarking with state-of-the-art 2D-FeFETs.

a, Benchmark of state-of-the-art 2D-material FeFETs showing on/off ratio and memory window (MW)18,19,20,21,22,23,24,25,26,28,29,30,31,32,33,34,35,36,37,38. b, Benchmark plot comparing the memory window efficiency and ferroelectric thickness among the reported 2D-FeFETs and our devices18,19,20,21,22,23,24,25,28,29,31,32,34,35,36,37.

Extended Data Fig. 4 Response current uniformity under generator operating conditions.

Comparison of 9 individual device currents to the average crossbar array current: measured after programming voltage (VP) a, 4.8 V and b, 6.0 V under generator conditions (tPW = 100 ns), with the read voltage (VD) swept from 0.05 V to 0.562 V in 2 mV increments.

Extended Data Fig. 5 Response current uniformity under discriminator operating conditions.

Current responses of 9 devices in the array under discriminator conditions: a, at 4.6 V and b, at 6.0 V bias voltages, with tPW = 100 µs. VD was swept from 0.05 to 0.306 V in 8-bit steps of 0.01 V.

Extended Data Fig. 6 Schematic of device-based deconvolution for pattern ‘N’.

a, Original 5×5 pattern padded to 7×7 size with zeros. b, The input matrix split into two matrices: one with positive values and another with negative values multiplied by –1. c, Two sets of 3×3 devices, programmed with the corresponding voltages and serving as kernels, are transposed and simultaneously used to perform operations with the input pattern. d, Pattern ‘N’ is derived from the final current response of the differential circuit formed by the two sub-arrays.

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Li, L., Li, C., Zheng, H. et al. Dual-mode ferroelectric transistors for high-performance generative-adversarial-network-based imaging. Nat. Sens. 1, 222–231 (2026). https://doi.org/10.1038/s44460-025-00024-w

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