Giant Light‐Heat‐Electricity Conversion in Photothermoelectric Detector Enabled by Semiconductor‐Dielectric Superlattices
Abstract
ABSTRACT Photothermoelectric (PTE) detectors, which operate relying on the photothermal and thermoelectric effects, can overcome the intrinsic spectral limitations originated from material bandgaps in photon‐driven detectors. However, the hardware implementation of devices leveraging light‐heat‐electricity cascade conversion remains challenging. Here, we report the construction of MoS 2 /SiO 2 semiconductor/dielectric superlattice films with features of nanoscale layer definition, high crystalline quality, and wafer‐level manufacturability. Benefiting from the interlayer interference and electric‐field localization, the MoS 2 /SiO 2 superlattices exhibit remarkably enhanced optical absorption across the visible to infrared spectrum, which enables the high photothermal energy conversion efficiency and substantial temperature rise exceeding 70 K. The PTE detection, implemented by integrating superlattice absorber with a microscale thermoelectric (μ‐TE) platform based on Bi 2 Te 3 /Sb 2 Te 3 P–N pairs, enables high‐efficiency photodetection through strong light–matter interaction and optimized thermal management. The self‐powered detector can stably operate over a broad‐spectrum range extending to 1550 nm, demonstrating a temporal response (∼16 ms), high responsivity (17.6 V W −1 ), and detectivity exceeding 1.20 × 10 10 Jones, comparable to state‐of‐the‐art broadband PTE detectors. Array‐level integration facilitates high‐fidelity 1550 nm imaging with a 256‐pixel prototype, while wafer‐scale fabrication of over 3000 units on a 2‐inch substrate confirms excellent uniformity, reproducibility and scalability, unlocking the potential for advanced large‐scale imaging applications.
Article Details
Authors (15)
Sheng Qiang
Ming‐Xin Zhang
School of Integrated Circuits Harbin Institute of Technology (Shenzhen) Shenzhen China
Jintao Wang
Bing‐Xuan Zhu
School of Integrated Circuits Harbin Institute of Technology (Shenzhen) Shenzhen China
Lin‐Qing Yue
Sauvage Laboratory for Smart Materials School of Materials Science and Engineering Harbin Institute of Technology (Shenzhen) Shenzhen China
Xu Pan
School of Integrated Circuits, Harbin Institute of Technology (Shenzhen) 1 , Shenzhen 518055,
Zhao Lei
Sauvage Laboratory for Smart Materials School of Materials Science and Engineering Harbin Institute of Technology (Shenzhen) Shenzhen China
Ruo‐Yao Sun
School of Integrated Circuits Harbin Institute of Technology (Shenzhen) Shenzhen China
Pei‐Yu Huang
School of Integrated Circuits Harbin Institute of Technology (Shenzhen) Shenzhen China
Qian Zhang
Wen‐Bo Duan
School of Integrated Circuits Harbin Institute of Technology (Shenzhen) Shenzhen China
Mingyu Li
Liang Zhen
School of Materials Science and Engineering
Jing‐Kai Qin
School of Integrated Circuits Harbin Institute of Technology (Shenzhen) Shenzhen China
Cheng‐Yan Xu
Sauvage Laboratory for Smart Materials School of Materials Science and Engineering Harbin Institute of Technology (Shenzhen) Shenzhen China