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首页> 外文期刊>ACS applied materials & interfaces >Energetics of Nonradiative Surface Trap States in Nanoparticles Monitored by Time-of-Flight Photoconduction Measurements on Nanoparticle-Polymer Blends
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Energetics of Nonradiative Surface Trap States in Nanoparticles Monitored by Time-of-Flight Photoconduction Measurements on Nanoparticle-Polymer Blends

机译:通过在纳米粒子 - 聚合物共混物上通过飞行时间光电电压测量监测的纳米粒子中的非地表面捕集状态的能量学

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Nanoparticles (NPs) have had increasingly successful applications including in emissive or photovoltaic devices; however, trap states associated with the surface of NPs often drastically reduce the efficiency of devices and are difficult to detect spectroscopically. We show the applicability of photoconduction as the means of detecting and quantifying trap states in NPs. We performed time-of-flight (ToF) photoconduction measurements, using semiconducting poly[bis(4-phenyl)(4-butyphenyl)amine] (P-TPD) doped with either core/shell CdSeS/CdS quantum dots (QDs) or perovskite CsPbBr3 NPs, both of which are carefully designed to be energetically matched. In the case of the QDs, a drop in the hole mobility from similar to 10(-3) to similar to 10(-4) cm(2) V-1 s(-1) was observed when compared to a control sample, suggesting the presence of a hole trapping. These trap states were found to be around -5.0 to -4.9 eV from the vacuum level. The presence of the trap states was further supported by a coincident reduction in the photoluminescence (PL), quantum yield (QY), and lifetime of the core/shell QDs after purification. Using the measured reductions in the PL, QY, and lifetime, the surface trap state density was estimated to increase by between 20 and 40%, most likely due to a ligand detachment. In the case of the perovskite NP-doped samples, a mobility of similar to 10(-3) cm(2) V-1 s(-1) was measured. Thus, doping with perovskite NPs did not generate any obvious hole trapping from the P-TPD matrix. The absence of a trapping may be related to the reduced surface-to-volume ratio and NP number density of the perovskite NPs compared to the core/shell QDs, since the perovskite NPs are approximately 10 times larger in radius than that of the core/shell QDs. Our results suggest that to minimize the presence of trap states with a view to improving device performance, large-size perovskite NPs appear to be better than small-size QDs.
机译:纳米颗粒(NPS)具有越来越成功的应用,包括在发光或光伏器件中;然而,与NPS表面相关的陷阱状态通常会大大降低设备的效率,并且难以检测光谱。我们展示了光电通电的适用性作为检测和量化NPS中陷阱状态的方法。我们使用掺杂有核/壳CDSE / CDS量子点(QDS)或掺杂有核/壳CDSES / CDS量子点(QDS)或Perovskite CSPBBR3 NPS,两者都经过精心设计,以便充满活力匹配。在QDS的情况下,与对照样品相比,观察到从类似于10(-3)至类似于10(-4)cm(2)厘米(2)v-1s(-1)的空穴迁移率的下降。建议存在漏洞。这些陷阱状态被发现从真空水平到-4.9 ev。通过在纯化后的光致发光(PL),量子产率(QY)和核心/壳QD的寿命的重合还原,进一步支持捕集状态的存在。利用PL,QY和寿命中的测量减少,估计表面捕集状态密度增加20%至40%,最有可能由于配体脱离而增加。在钙钛矿NP掺杂样品的情况下,测量类似于10(-3)cm(2)厘米(-1)的迁移率。因此,掺杂与Perovskite NP没有从P-TPD矩阵产生任何明显的孔捕获。与核心/壳QD相比,缺失捕获可能与钙钛矿NP的降低的表面到体积比和NP数密度有关,因为钙钛矿NPS的半径大约比核心的大约10倍。壳QD。我们的结果表明,为了最大限度地减少陷阱状态的存在,以提高器件性能,大尺寸的Perovskite NPS似乎比小尺寸的QD更好。

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