Dual passivation effect of a C60-capped and Zn2+-doped CsPbCl3 perovskite photodetector†
Abstract
In this study, the divalent metal dopant cation of Zn2+ and a surface capping layer of C60 were simultaneously incorporated into a CsPbCl3 perovskite on an Si/SiO2 substrate, and the photoresponse performance of the CsPbCl3-based photodetector was investigated. It was found that the doping ratio of ZnCl2 and thickness of the C60 capping layer exhibited significant influences on the photophysical features and photoresponse performances. With the optimal Zn2+ ratio of 11.0% and C60 layer thickness of 10 nm, a wide wavelength range photoresponse from UV to NIR (350–1010 nm) was achieved with the optimal responsivity (R), detectivity D* and noise equivalent power (NEP) of 10 477 A W−1, 2.09 × 1014 Jones (cm Hz1/2 W−1) and 4.16 × 10−10 W Hz−1/2, respectively, at the incident light wavelength (λ) of 500 nm and 0.2 mW cm−2 power. Meanwhile, the dependence of trap density and carrier mobility on Zn2+ concentration and C60 layer thickness derived from the mode of space charge limited current (SCLC) with the lowest and highest values of 3.2 × 1015 cm−3 and 1.52 × 10−3 cm2 V−1 s−1, respectively, at the optimal Zn2+ doping ratio and C60 layer thickness demonstrated a dual-passivation effect from both Zn2+ and C60. Such behavior may be attributed to the interaction between the A and B site species in the C60-capped and Zn2+-doped CsPbCl3, promoting the suppression of defects and restoration of structure. Meanwhile, the exciton binding energy (EB) imposed a critical impact on the carrier dynamics and PL performance. Thus, the photoresponse is controlled by the combining effects of structure defects and exciton binding energy, both of which can be strongly modulated by the ZnCl2 doping concentration and C60 capping layer thickness.