Study on the effect of non-fullerene doping on the photoelectric properties of planar heterojunction organic photodetectors
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摘要:
本论文研究了在P3HT : PC71BM 的平面异质结有机光电探测器体系中掺杂非富勒烯小分子IEICO-4F到受体部分对该器件光电特性的影响。本实验采用溶液法制备不同掺杂比例的活性层薄膜,通过电流-电压特性、外量子效率、紫外-可见-近红外吸收光谱及光致发光光谱等表征手段,结合原子力显微镜分析形貌演变规律。实验研究表明,IEICO-4F 的引入显著拓宽活性层吸收光谱,拓宽至近红外区域(700~900 nm),并通过互补吸收光谱提升光量子捕获效率。当优化掺杂比例为30% 时,器件的光电流密度从19.17 mA/cm2提升至27.25 mA/cm2,比探测率从0.78×1012 Jones 提升到1.45×1012 Jones。形貌分析证实 IEICO-4F 优化了 PC71BM 的相分布,形成更精细的互穿网络结构,促进电荷转移并降低串联电阻,研究同时发现过量掺杂会破坏相分离平衡,影响载流子分离和流入,导致电子-空穴的传输不平衡。该工作揭示了非富勒烯受体掺杂对传统聚合物——富勒烯体系的多重调控作用。研究发现通过光谱拓宽与形貌优化的协同机制可有效提升器件光电性能,为有机光电探测材料体系的设计提供了新思路。
Abstract:This study investigates the impact of doping the non-fullerene small molecule IEICO-4F into the acceptor component of a planar heterojunction organic photodetector based on the P3HT : PC71BM system on the device's optoelectronic properties. The active layer films with different doping ratios were fabricated using a solution process. Characterization techniques including current-voltage measurements, external quantum efficiency, ultraviolet-visible-near-infrared absorption spectroscopy, and photoluminescence spectroscopy were employed, combined with atomic force microscopy to analyze morphological evolution. Experimental results demonstrate that the introduction of IEICO-4F significantly broadens the absorption spectrum of the active layer into the near-infrared region (700−900 nm) and enhances photon capture efficiency through complementary absorption spectrum. At an optimized doping ratio of 30%, the device's photocurrent density increased from 19.17 mA/cm2 to 27.25 mA/cm2, and the specific detectivity improved from 0.78×1012 Jones to 1.45×1012 Jones. Morphological analysis confirmed that IEICO-4F optimizes the phase distribution of PC71BM, forming a finer interpenetrating network structure that facilitates charge transfer and reduces series resistance. The study also revealed that excessive doping disrupts the phase separation balance, adversely affecting carrier separation and transport, leading to an imbalance in electron-hole transport. This work highlights the multifaceted regulatory effect of non-fullerene acceptor doping on traditional polymer: fullerene systems, effectively enhancing device performance through the synergistic mechanisms of spectral broadening and morphological optimization, thereby providing new insights for the design of organic photodetector material systems.
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图 2 (a) 活性层三种材料的归一化吸收;(b) 器件活性层的归一化吸收;(c) 在光照条件下,不同IEICO-4F掺杂浓度的器件所呈现的电流密度-电压响应特性;(d) 在暗条件下,不同IEICO-4F掺杂浓度的器件所呈现的电流密度-电压响应特性
Figure 2. (a) Normalized absorption of the three materials in the active layer; (b) normalized absorption of the device's active layer; (c) current density-voltage characteristics of devices with different IEICO-4F doping concentrations under illumination; (d) current density-voltage characteristics of devices with different IEICO-4F doping concentrations under dark conditions
图 6 (a) 无掺杂的RMS图;(b) 30%的IEICO-4F掺杂下的RMS图;(c) 50%的IEICO-4F掺杂下的RMS图;(d) 无掺杂的相图;(e) 30%的IEICO-4F掺杂下的相图;(f) 50%的IEICO-4F掺杂下的相图
Figure 6. (a) RMS map of undoped system; (b) RMS map with 30% IEICO-4F doping; (c) RMS map with 50% IEICO-4F doping; (d) phase diagram of the undoped system; (e) phase diagram with 30% IEICO-4F doping; (f) phase diagram with 50% IEICO-4F doping
表 1 在−0.1 V下,不同IEICO-4F掺杂比例时器件的性能参数
Table 1. Performance parameters of the device under different doping ratios of IEICO-4F at −0.1 V
Jph
(×10−1 mA/cm2)Jd
(×10−3 mA/cm2)R
(mA/W)D*
(×1012 Jones)Control 2.32 (±0.35) 8.88 (±0.32) 214.3 (±0.01) 1.37 (±0.18) 10% 3.62 (±0.42) 4.39 (±0.27) 349.1 (±0.03) 2.99 (±0.25) 30% 4.50 (±0.39) 3.74 (±0.18) 437.7 (±0.01) 4.14 (±0.14) 50% 3.81 (±0.34) 37.79 (±0.22) 373.5 (±0.02) 1.21 (±0.11) 表 2 不同IEICO-4F掺杂比例下的器件阻抗参数
Table 2. Device’s impedance parameters under different IEICO-4F doping ratios
R1/Ω R2/Ω C/F Control 83.24 2.66×105 1.28×10−9 30% 77.31 2.01×105 1.34×10−9 表 3 不同IEICO-4F掺杂比例下的器件载流子迁移率
Table 3. Device carrier mobility under different IEICO-4F doping ratios
µh(cm2/Vs) µe(cm2/Vs) µe/µh Control 2.38×10−4 1.35×10−4 0.57 30% 2.79×10−4 1.72×10−4 0.62 -
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