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Spatial and Intensity Modulation of Nanowire Emission Induced by Mobile Charges

机译:移动电荷引起的纳米线发射的空间和强度调节

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摘要

Single-molecule optical experiments carried out in conjunction with externally applied electric fields show deliberate spatial and intensity control over CdSe nanowire (NW) emission. In particular, by applying external fields to electrically isolated (single) NWs, their emission can be localized in areas of the wire closest to the positive electrode. In a few cases, the resulting emission intensity increases over the corresponding zero-field value by nearly an order of magnitude. More often than not, factors of 2-3 are seen. Reversing the field polarity causes the emission to localize in opposite regions of the wire. Emission from individual NWs can therefore be modulated. Complementary ac electric field measurements show that the effect persists up to 500 kHz. To explain the phenomenon, the effective passivation of surface trap states by mobile carriers is speculated. This, in turn, causes local changes in the NW emission quantum yield (QY). To verify the presence of such mobile charges, both ensemble and single NW bundle electrophoresis experiments are conducted. By investigating subsequent NW rotational and translational dynamics, an estimate for the number of mobile carriers is determined. A lower limit (best case) linear charge density of ~0.45-1.2 mobile electrons per micrometer of the wire is obtained. Apart from self-consistently explaining the field-induced NW emission modulation, the resulting data and subsequent analysis also suggests that the same mobile carriers may be the root cause of NW emission intermittency. Furthermore, given the ubiquity of stray charges, the resulting hypothesis may have additional applicability toward explaining blinking in other systems, a problem of current interest especially within the context of colloidal QDs.
机译:结合外部施加的电场进行的单分子光学实验表明,对CdSe纳米线(NW)发射进行了有意的空间和强度控制。特别地,通过将​​外部场施加到电隔离的(单个)NW,其发射可以被定位在最靠近正极的导线区域中。在某些情况下,最终的发射强度会在相应的零场值上增加近一个数量级。通常会看到2-3的因子。反转场极性会导致发射定位在导线的相对区域。因此,可以调制来自各个NW的发射。互补的交流电场测量表明,这种影响一直持续到500 kHz。为了解释该现象,推测了移动载流子对表面陷阱状态的有效钝化。反过来,这会导致NW发射量子产率(QY)发生局部变化。为了验证这种移动电荷的存在,进行了集成和单个NW束电泳实验。通过研究随后的西北旋转和平移动力学,可以确定移动载波数量的估计值。获得的下限(最佳情况下)为每微米导线约〜0.45-1.2移动电子线性电荷密度。除了自洽地解释磁场引起的NW发射调制之外,所得数据和后续分析还表明,相同的移动载波可能是NW发射间歇性的根本原因。此外,考虑到杂散电荷的普遍存在,所得到的假设可能对解释其他系统中的闪烁具有额外的适用性,这是当前关注的问题,尤其是在胶体量子点的情况下。

著录项

  • 来源
    《Journal of the American Chemical Society》 |2007年第43期|13160-13171|共12页
  • 作者单位

    Department of Chemistry and Biochemistry, Notre Dame Radiation Laboratory, University of Notre Dame, Notre Dame, Indiana 46556;

  • 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
  • 中图分类 化学;
  • 关键词

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