Nguyen Huy A, Srivastava Indrajit, Pan Dipanjan, Gruebele Martin
Mills Breast Cancer Institute, Carle Foundation Hospital, 509 West University Avenue, Urbana, Illinois 61801, United States.
Carle Illinois College of Medicine, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, United States.
ACS Nano. 2020 May 26;14(5):6127-6137. doi: 10.1021/acsnano.0c01924. Epub 2020 Apr 28.
Unlike quantum dots, photophysical properties of carbon dots (CDs) are not strongly correlated with particle size. The origin of CD photoluminescence has been related to sp domain size and the abundance of oxidized surface defects. However, direct imaging of surface-accessible spatially localized oxidized defects is still lacking. In this work, solvothermal-synthesized CDs are fractionated into different colors by polarity-based chromatography. We then study the mechanism of CD fluorescence by directly imaging individual CDs with subparticle resolution by scanning tunneling microscopy. Density of states imaging of CDs reveals that the graphitic core has a large bandgap that is inconsistent with observed fluorescence wavelength, whereas localized defects have smaller electronic gaps for both red-emitting dots (rCDs) and blue-emitting dots (bCDs). For individual bCDs within our laser tuning range, we directly image optically active surface defects (. 1-3 nm in size) and their bandgaps, which agree with the emission wavelength of the ensemble from which the bCDs were taken. We find that the emissive defects are not necessarily the ones with the smallest gap, consistent with quantum yields less than unity (0.1-0.26). X-ray photoelectron spectroscopy and pH-dependent fluorescence titration show that oxygen-containing surface-accessible protonatable functional groups (e.g., phenolic -OH, -COOH) define the chemical identity of the defects. This observation explains why we detect neither long-lived optical excitation of the core nor a correlation between size and emission wavelength. Instead, control over the number of oxygen-containing defects defines the emission wavelength, with more oxidized defects at the surface producing redder emission wavelengths.
与量子点不同,碳点(CDs)的光物理性质与粒径没有很强的相关性。CD光致发光的起源与sp域尺寸和氧化表面缺陷的丰度有关。然而,仍然缺乏对表面可及的空间局域氧化缺陷的直接成像。在这项工作中,通过基于极性的色谱法将溶剂热合成的CDs分离成不同颜色。然后,我们通过扫描隧道显微镜以亚颗粒分辨率对单个CDs进行直接成像,研究CD荧光的机制。CDs的态密度成像表明,石墨核具有与观察到的荧光波长不一致的大带隙,而局域缺陷对于红色发射点(rCDs)和蓝色发射点(bCDs)具有较小的电子能隙。对于我们激光调谐范围内的单个bCDs,我们直接成像光学活性表面缺陷(尺寸为1 - 3 nm)及其带隙,这与从中获取bCDs的整体发射波长一致。我们发现发射缺陷不一定是能隙最小的缺陷,这与小于1(0.1 - 0.26)的量子产率一致。X射线光电子能谱和pH依赖的荧光滴定表明,含表面可及的可质子化含氧官能团(例如,酚羟基 -OH、-COOH)定义了缺陷的化学特性。这一观察结果解释了为什么我们既没有检测到核的长寿命光学激发,也没有检测到尺寸与发射波长之间的相关性。相反,对含氧缺陷数量的控制决定了发射波长,表面氧化缺陷越多,发射波长越红。