首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Ultrafast Charge Carrier Delocalization in CdSe/CdS Quasi-Type ll and CdS/CdSe Inverted Type I Core-Shell: A Structural Analysis through Carrier-Quenching Study
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Ultrafast Charge Carrier Delocalization in CdSe/CdS Quasi-Type ll and CdS/CdSe Inverted Type I Core-Shell: A Structural Analysis through Carrier-Quenching Study

机译:CdSe / CdS拟II型和CdS / CdSe倒置I型核壳的超快电荷载流子离域:通过载流子猝灭研究的结构分析

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We have employed femtosecond transient absorption spectrocopy to monitor charge carrier delocalization in CdSe/CdS quasi-type II and CdS/CdSe inverted type I core-shell nanocrystals (NCs). Interestingly, CdSe and CdS QD pairs can make both type I and quasi-type II core-shell structures, depending on their band alignment and charge carrier localization. Steady-state optical absorption and luminescence studies show a gradual red-shift in both optical absorption and emission spectra in CdSe/CdS core-shell with increasing CdS shell thickness. The luminescence quantum yield in CdSe/CdS core-shell drastically increases with shell thickness. Notably, CdS/CdSe inverted core-shell shows a huge red-shift both in absorption and luminescence which closely matches with the band edge photoluminescence (PL) of pure CdSe QDs (shell). However, the luminescence quantum yield does not change much with shell thickness. Depending on their band energy level alignment, the charge carrier (electron and hole) delocalization in both the core-shells have been demonstrated using electron (benzoquinone, BQ) and hole (pyridine, Py) quencher. The bleach recovery kinetics of CdS/CdSe core-shell recovers faster in the presence of both BQ and Py. However, for CdSe/CdS core-shell, the bleach recovers faster only in the presence of BQ while the bleach dynamics remain unaffected in the presence of Py. Our experimental observations suggest that in CdSe/CdS quasi-type II core-shell, photoexcited electrons are localized in CdS shell and holes are localized in CdSe core; however, in CdS/CdSe inverted core-shell both electrons and holes are localized in the CdSe shell.
机译:我们已采用飞秒瞬态吸收光谱法来监测CdSe / CdS准II型和CdS / CdSe倒I型核-壳纳米晶体(NCs)中的载流子离域。有趣的是,CdSe和CdS QD对可以形成I型和准II型核-壳结构,这取决于它们的能带排列和电荷载流子定位。稳态光吸收和发光研究表明,随着CdS壳厚度的增加,CdSe / CdS核壳的光吸收和发射光谱均出现逐渐的红移。 CdSe / CdS核壳中的发光量子产率随壳厚度的增加而急剧增加。值得注意的是,CdS / CdSe倒置的核-壳在吸收和发光方面均显示出巨大的红移,与纯CdSe QD(壳)的带边缘光致发光(PL)紧密匹配。但是,发光量子产率不会随着壳的厚度而改变很多。取决于它们的能带能级排列,已经使用电子(苯醌,BQ)和空穴(吡啶,Py)猝灭剂证明了两个核壳中的载流子(电子和空穴)离域化。在同时存在BQ和Py的情况下,CdS / CdSe核壳的漂白剂恢复动力学恢复得更快。但是,对于CdSe / CdS核壳,只有在存在BQ的情况下,漂白剂才能更快地恢复,而在存在Py的情况下,漂白剂动力学不会受到影响。我们的实验观察表明,在CdSe / CdS准II型核-壳中,光激发电子位于CdS壳中,而空穴位于CdSe核中。然而,在CdS / CdSe倒置的核壳中,电子和空穴都位于CdSe壳中。

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