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具有浓度依赖表面结构的胶体量子点配体吸附模型。

Model for adsorption of ligands to colloidal quantum dots with concentration-dependent surface structure.

机构信息

Department of Chemistry, Northwestern University, 2145 Sheridan Road, Evanston, Illinois 60208-3113, USA.

出版信息

ACS Nano. 2012 Jan 24;6(1):557-65. doi: 10.1021/nn203950s. Epub 2011 Dec 7.

Abstract

A study of the adsorption equilibrium of solution-phase CdS quantum dots (QDs) and acid-derivatized viologen ligands (N-[1-heptyl],N'-[3-carboxypropyl]-4,4'-bipyridinium dihexafluorophosphate, V(2+)) reveals that the structure of the surfaces of the QDs depends on their concentration. This adsorption equilibrium is monitored through quenching of the photoluminescence of the QDs by V(2+) upon photoinduced electron transfer. When modeled with a simple Langmuir isotherm, the equilibrium constant for QD-V(2+) adsorption, K(a), increases from 6.7 × 10(5) to 8.6 × 10(6) M(-1) upon decreasing the absolute concentration of the QDs from 1.4 × 10(-6) to 5.1 × 10(-8) M. The apparent increase in K(a) upon dilution results from an increase in the mean number of available adsorption sites per QD from 1.1 (for [QD] = 1.4 × 10(-6) M) to 37 (for [QD] = 5.1 × 10(-8) M) through desorption of native ligands from the surfaces of the QDs and through disaggregation of soluble QD clusters. A new model based on the Langmuir isotherm that treats both the number of adsorbed ligands per QD and the number of available binding sites per QD as binomially distributed quantities is described. This model yields a concentration-independent value for K(a) of 8.7 × 10(5) M(-1) for the QD-V(2+) system and provides a convenient means for quantitative analysis of QD-ligand adsorption in the presence of competing surface processes.

摘要

研究表明,溶液相 CdS 量子点(QD)和酸衍生化的紫精配体(N-[1-庚基],N'-[3-羧基丙基]-4,4'-联吡啶二六氟磷酸酯,V(2+))的吸附平衡取决于 QD 的浓度。通过光诱导电子转移过程中 V(2+)对 QD 光致发光的猝灭来监测这种吸附平衡。当用简单的 Langmuir 等温线进行建模时,QD-V(2+)吸附的平衡常数 K(a)从 6.7×10(5)增加到 8.6×10(6) M(-1),这是由于 QD 的绝对浓度从 1.4×10(-6)降低到 5.1×10(-8) M。稀释时 K(a)的表观增加是由于每个 QD 的可用吸附位点的平均数量从 1.1(对于 [QD] = 1.4×10(-6) M)增加到 37(对于 [QD] = 5.1×10(-8) M),这是通过从 QD 表面解吸天然配体和通过可溶 QD 团簇的解聚来实现的。描述了一种基于 Langmuir 等温线的新模型,该模型将每个 QD 上吸附的配体数量和每个 QD 上的可用结合位点数量都视为二项分布的数量。该模型为 QD-V(2+)体系提供了一个与浓度无关的 K(a)值 8.7×10(5) M(-1),并为在存在竞争表面过程的情况下进行 QD-配体吸附的定量分析提供了一种方便的方法。

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