Han Zeyao, Fu Weifei, Zou Yousheng, Gu Yu, Liu Jiaxin, Huang Bo, Yu Dejian, Cao Fei, Li Xiaoming, Xu Xiaobao, Zeng Haibo
Key Laboratory of Advanced Display Materials and Devices, Ministry of Industry and Information Technology, Institute of Optoelectronics and Nanomaterials, School of Material Science and Engineering, Nanjing University of Science and Technology, Nanjing, 210094, China.
Department of Materials Science, Technical University of Darmstadt, Darmstadt, 64287, Germany.
Adv Mater. 2021 Mar;33(11):e2003852. doi: 10.1002/adma.202003852. Epub 2021 Feb 8.
Photodetectors selective to the polarization empower breakthroughs in sensing technology for target identification. However, the realization of polarization-sensitive photodetectors based on intrinsically anisotropic crystal structure or extrinsically anisotropic device pattern requires complicated epitaxy and etching processes, which limit scalable production and application. Here, solution-processed PEA MA (Sn Pb ) I (PEA= phenylethylammonium, MA= methylammonium) polycrystalline film is probed as photoactive layer toward sensing polarized photon from 300 to 1050 nm. The growth of the PEA MA (Sn Pb ) I crystal occurs in confined crystallographic orientation of the (202) facet upon the assistance of NH SCN and NH Cl, enhancing anisotropic photoelectric properties. Therefore, the photodetector achieves a polarization ratio of 0.41 and dichroism ratio (I /I ) of 2.4 at 900 nm. At 520 nm, the I /I even surpasses the one of the perovskite crystalline films, 1.8 and ≈1.2, respectively. It is worth noting that the superior figure-of-merits possess a response width of 900 kHz, I /I ratio of ≈3 × 10 , linear dynamic range from 0.15 nW to 12 mW, noise current of 8.28 × 10 A × Hz , and specific detectivity of 1.53 × 10 Jones, which demonstrate high resolution and high speed for weak signal sensing and imaging. The proof of concept in polarized imaging confirms that the polarization-sensitive photodetector meets the requirements for practical application in target recognition.
对偏振具有选择性的光电探测器推动了用于目标识别的传感技术取得突破。然而,基于本征各向异性晶体结构或非本征各向异性器件图案来实现偏振敏感型光电探测器,需要复杂的外延和蚀刻工艺,这限制了可扩展生产及应用。在此,溶液处理的苯乙胺甲脒(锡铅)碘化物(苯乙胺 = 苯乙铵,甲脒 = 甲铵)多晶膜被用作光活性层,用于探测300至1050纳米的偏振光子。在硫氰酸铵和氯化铵的辅助下,苯乙胺甲脒(锡铅)碘化物晶体在(202)面的受限晶体取向中生长,增强了各向异性光电性能。因此,该光电探测器在900纳米处实现了0.41的偏振比和2.4的二向色比(I⊥/I∥)。在520纳米处,I⊥/I∥甚至分别超过了钙钛矿晶体薄膜的1.8和≈1.2。值得注意的是,该探测器具有出色的品质因数,响应宽度为900千赫兹,I⊥/I∥比约为3×10,线性动态范围为0.15纳瓦至12毫瓦,噪声电流为8.28×10−12安培·赫兹−1/2,比探测率为1.53×1012琼斯,这表明其在弱信号传感和成像方面具有高分辨率和高速度。偏振成像中的概念验证证实,偏振敏感型光电探测器满足目标识别实际应用的要求。