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Time-Resolved Studies of Fluorescence and Band-Edge Charge Carriers Dynamics in In_(1-x)Ga_xP Colloidal Quantum Dots

机译:In_(1-x)Ga_xP胶体量子点中荧光和带边电荷载流子动力学的时间分辨研究

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In this submission, we report on the results of spectroscopic studies of charge carrier dynamics in colloidal In_(1-x)Ga_xP quantum dots (QDs) with low levels of Ga doping (x ~1%). These QDs exhibit large global Stokes shift of fluorescence (up to 300 meV) along with high emission yield (up to 30% in solution and 25% in films under blue excitation at 300 K) after post-synthesis photo-chemical treatment. In order to reveal the nature of large fluorescence Stokes shift and study the band-edge carriers dynamics, we performed time-resolved measurements of emission and photo-induced absorption changes in QDs with different sizes and surface passivation. The work was focused on the studies of differences between QDs subjected to photochemical surface passivation and bare nanoparticles. Time-resolved absorption spectroscopy indicates that holes' trapping strongly depends on passivation of surface trap states and can even suppress Auger multiparticle recombination in poorly passivated nanoparticles. Transient fluorescence measurements in well-passivated nanoparticles demonstrate that at short delays (<2 ns), emission Stokes shift is almost twice smaller than in steady-state measurements and matches the emission band in unpassivated QDs. At longer delays, time-resolved emission matches the spectra obtained with continuous wave (CW) excitation. We propose that initially photoluminescence occurs from quantum-confined state and subsequent hole relaxation onto surface/interface sites gives rise to emission with large global Stokes shift. In poorly passivated QDs, holes escape quickly to deep-trap states that leads to formation of low-efficiency broad emission band red-shifted with respect to the excitonic PL band.
机译:在本文中,我们报道了在Ga掺杂水平低(x〜1%)的In_(1-x)Ga_xP胶体量子点(QDs)中的载流子动力学的光谱研究结果。合成后的光化学处理后,这些量子点表现出大的全局斯托克斯位移荧光(高达300 meV)以及高发射率(在300 K的蓝色激发下溶液中高达30%,薄膜中膜高达25%)。为了揭示大荧光斯托克斯位移的性质并研究带边载流子的动力学,我们对不同尺寸和表面钝化的量子点进行了发射和光诱导吸收变化的时间分辨测量。这项工作集中在研究光化学表面钝化的量子点与裸露的纳米粒子之间的差异。时间分辨吸收光谱表明,空穴的俘获在很大程度上取决于表面俘获态的钝化,甚至可以抑制钝化不良的纳米粒子中的俄歇多粒子复合。钝化良好的纳米颗粒中的瞬态荧光测量结果表明,在短延迟(<2 ns)下,发射斯托克斯位移几乎是稳态测量结果的两倍,并且与未钝化QD中的发射带相匹配。在较长的延迟下,时间分辨的发射与连续波(CW)激发获得的光谱匹配。我们提出,最初的光致发光是从量子约束状态发生的,随后空穴在表面/界面位点上的弛豫产生了具有大全局斯托克斯位移的发射。在钝化差的量子点中,空穴迅速逃逸到深陷阱状态,这导致形成低效率的宽发射带,相对于激子PL带红移。

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