Shows enhanced polarity modulation in optoelectronic devices, suggesting improved sensing capabilities.
Next‐generation intelligent vision systems demand not only high‐fidelity sensing but also in‐sensor processing that is fast, adaptive, and energy‐efficient. Existing in‐sensor paradigms ignore photocurrent polarity—an intrinsic decision variable—forcing computation into amplitude thresholds or multi‐device pipelines. Here, we present a polarity‐programmable optoelectronic device based on bipolar‐barrier heterostructures equipped separately with vertical and horizontal channels. By exploiting the interplay between bipolar barriers, the device enables modulation of photocurrent polarity—realizing dynamic ternary‐state output (‘−1’, ‘0’, ‘+1’) governed solely by laser position, bias voltage, wavelength, and power‐ coded. The vertical structure exhibits a bipolar response with an ultralow switching bias of −0.025 V (less than 1/10 that of the horizontal structure), along with wavelength‐tunable polarity, a responsivity of 0.22 A/W, a detectivity of 8.6 × 10 9 cm Hz 1/2 W −1 , and a fast response time of ∼ 121 µs due to its large photosensitive area, shortened carrier transport, and wavelength‐dependent optical field distribution. Programming wavelength and power density enable a single device to deterministically realize all Boolean gates, polarity‐resolved imaging, and visible‐infrared dual‐channel transmission. This multidimensional polarity‐programmable pathway in bipolar‐barrier heterojunctions intrinsically integrates sensing, signal encoding, and logic operations within a single physical unit, establishing polarity programming as a scalable paradigm for optoelectronic computing.
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Mi et al. (2026) studied this question.
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