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Mid-Gap States and Normal vs Inverted Bonding in Luminescent Cu~+- and Ag~+-Doped CdSe Nanocrystals

机译:掺杂Cu〜+和Ag〜+的CdSe纳米晶体的中间能隙态和正态键与反向键

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摘要

Mid-gap luminescence in copper (Cu~+)-doped semiconductor nanocrystals (NCs) involves recombination of delocalized conduction-band electrons with copper-localized holes. Silver (Ag~+)-doped semiconductor NCs show similar mid-gap luminescence at slightly (~0.3 eV) higher energy, suggesting a similar luminescence mechanism, but this suggestion appears inconsistent with the large difference between Ag~+ and Cu~+ ionization energies (~1.5 eV), which should make hole trapping by Ag~+ highly unfavorable. Here, Ag~+-doped CdSe NCs (Ag~+:CdSe) are studied using time-resolved variable-temperature photoluminescence (PL) spectroscopy, magnetic circularly polarized luminescence (MCPL) spectroscopy, and time-dependent density functional theory (TD-DFT) to address this apparent paradox In addition to confirming that Ag~+:CdSe and Cu~+:CdSe NCs display similar broad PL with large Stokes shifts, we demonstrate that both also show very similar temperature-dependent PL lifetimes and magneto-luminescence. Electronic-structure calculations further predict that both dopants generate similar localized mid-gap states. Despite these strong similarities, we conclude that these materials possess significandy different electronic structures. Specifically, whereas photogenerated holes in Cu~+:CdSe NCs localize primarily in Cu(3d) orbitals, formally oxidizing Cu~+ to Cu~(2+), in Ag~+:CdSe NCs they localize primarily in 4p orbitals of the four neighboring Se~(2-) ligands, and Ag~+ is not oxidized. This difference reflects a shift from "normal" to "inverted" bonding going from Cu~+ to Ag~+. The spectroscopic similarities are explained by the fact that, in both materials, photogenerated holes are localized primarily within covalent [MSe_4] dopant clusters (M = Ag~+, Cu~+). These findings reconcile the similar spectroscopies of Ag~+- and Cu~+-doped semiconductor NCs with the vastly different ionization potentials of their Ag~+ and Cu~+ dopants.
机译:掺杂铜(Cu〜+)的半导体纳米晶体(NC)中的中间能隙发光涉及离域导带电子与铜局部空穴的复合。掺杂银(Ag〜+)的半导体NC在稍高(〜0.3 eV)的能量下显示出相似的中间能隙发光,表明了相似的发光机理,但这与Ag〜+和Cu〜+的电离之间的巨大差异相矛盾。能量(〜1.5 eV),这将非常不利于Ag〜+俘获空穴。在这里,使用时间分辨的可变温度光致发光(PL)光谱,磁圆极化发光(MCPL)光谱和随时间变化的密度泛函理论(TD-)对Ag〜+掺杂的CdSe NCs(Ag〜+:CdSe)进行了研究。 DFT)以解决这一明显的悖论除了确认Ag〜+:CdSe和Cu〜+:CdSe NCs具有相似的宽PL和大Stokes位移外,我们还证明了它们还显示出非常相似的温度依赖性PL寿命和磁致发光。电子结构计算进一步预测两种掺杂剂均会产生相似的局部中间能隙状态。尽管存在这些相似之处,但我们得出的结论是,这些材料具有明显不同的电子结构。具体来说,尽管Cu〜+:CdSe NCs中的光生空穴主要位于Cu(3d)轨道,形式上将Cu〜+氧化为Cu〜(2+),而在Ag〜+:CdSe NCs中,Cu_ +正式氧化为Cu〜(2+),但它们主要位于四个的4p轨道邻近的Se〜(2-)配体,而Ag〜+不被氧化。这种差异反映了从Cu〜+到Ag〜+从“正常”键向“反向”键的转变。光谱上的相似性是由以下事实解释的:在两种材料中,光生空穴主要位于共价[MSe_4]掺杂剂簇(M = Ag〜+,Cu〜+)中。这些发现使Ag〜+和Cu〜+掺杂的半导体NC的相似光谱与它们的Ag〜+和Cu〜+掺杂剂的巨大电离势相一致。

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  • 来源
    《Journal of the American Chemical Society》 |2017年第18期|6411-6421|共11页
  • 作者单位

    Department of Chemistry, University of Washington, Seattle, Washington 98195-1700, United States;

    Department of Chemistry, University of Washington, Seattle, Washington 98195-1700, United States;

    Department of Chemistry, University of Washington, Seattle, Washington 98195-1700, United States;

    Department of Chemistry, University of Washington, Seattle, Washington 98195-1700, United States;

    Department of Chemistry, University of Washington, Seattle, Washington 98195-1700, United States;

    Department of Chemistry, University of Washington, Seattle, Washington 98195-1700, United States;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-18 03:07:57

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