Liu Haiqing, Han Jinkyu, McBean Coray, Lewis Crystal S, Kumar Routh Prahlad, Cotlet Mircea, Wong Stanislaus S
Department of Chemistry, State University of New York at Stony Brook, Stony Brook, NY 11794-3400, USA.
Condensed Matter of Physics and Materials Sciences Division, Brookhaven National Laboratory, Building 480, Upton, NY 11973, USA.
Phys Chem Chem Phys. 2017 Jan 18;19(3):2153-2167. doi: 10.1039/c6cp07648c.
Understanding the key parameters necessary for generating uniform Er,Yb co-activated NaYF possessing various selected phases (i.e. cubic or hexagonal) represents an important chemical strategy towards tailoring optical behavior in these systems. Herein, we report on a straightforward hydrothermal synthesis in which the separate effects of reaction temperature, reaction time, and precursor stoichiometry in the absence of any surfactant were independently investigated. Interestingly, the presence and the concentration of NHOH appear to be the most critical determinants of the phase and morphology. For example, with NHOH as an additive, we have observed the formation of novel hierarchical nanowire bundles which possess overall lengths of ∼5 μm and widths of ∼1.5 μm but are composed of constituent component sub-units of long, ultrathin (∼5 nm) nanowires. These motifs have yet to be reported as distinctive morphological manifestations of fluoride materials. The optical properties of as-generated structures have also been carefully analyzed. Specifically, we have observed tunable, structure-dependent energy transfer behavior associated with the formation of a unique class of NaYF-CdSe quantum dot (QD) heterostructures, incorporating zero-dimensional (0D), one-dimensional (1D), and three-dimensional (3D) NaYF structures. Our results have demonstrated the key roles of the intrinsic morphology-specific physical surface area and porosity as factors in governing the resulting opto-electronic behavior. Specifically, the trend in energy transfer efficiency correlates well with the corresponding QD loading within these heterostructures, thereby implying that the efficiency of FRET appears to be directly affected by the amount of QDs immobilized onto the external surfaces of the underlying fluoride host materials.
了解生成具有各种选定相(即立方相或六方相)的均匀铒、镱共激活的氟化钠钇所需的关键参数,是调整这些体系光学行为的重要化学策略。在此,我们报道了一种简单的水热合成方法,其中在没有任何表面活性剂的情况下,独立研究了反应温度、反应时间和前驱体化学计量比的单独影响。有趣的是,氢氧化钠的存在和浓度似乎是相和形态的最关键决定因素。例如,以氢氧化钠作为添加剂,我们观察到形成了新型的分级纳米线束,其总长度约为5μm,宽度约为1.5μm,但由长的超薄(约5nm)纳米线组成的组成亚单元构成。这些结构尚未作为氟化物材料独特的形态表现被报道。还仔细分析了所生成结构的光学性质。具体而言,我们观察到与形成一类独特的氟化钠钇-硒化镉量子点(QD)异质结构相关的可调谐、结构依赖的能量转移行为,该异质结构包含零维(0D)、一维(1D)和三维(3D)的氟化钠钇结构。我们的结果表明了固有形态特异性物理表面积和孔隙率作为控制所得光电行为的因素的关键作用。具体而言,能量转移效率的趋势与这些异质结构内相应的量子点负载量密切相关,从而意味着荧光共振能量转移(FRET)的效率似乎直接受到固定在底层氟化物主体材料外表面上的量子点数量的影响。