在Au102(p-MBA) 44集群的电子和振动签名
Eero Hulkko1, Olga Lopez-Acevedo, Jaakko Koivisto
1Nanoscience Center, Department of Chemistry, P.O. Box 35, FI-40014 University of Jyväskylä, Finland.
Journal of the American Chemical Society
|February 26, 2011
概括
测量和计算金纳米集群的光学吸收,揭示了关键的电子过渡. 合物交换没有影响核心电子属性,为未来的纳米集群应用提供了基准.
科学领域:
- 纳米技术纳米技术
- 材料科学 材料科学 材料科学
- 物理化学 物理化学
背景情况:
- 金纳米集群对各种应用具有前景.
- 了解它们的光学特性对于开发至关重要.
- 甲基酸 (p-MBA) 是一种常见的黄金纳米集群的连接体.
研究的目的:
- 测量和计算一个特定的黄金纳米集群的光学吸收光谱,Au{102}{p-MBA}{44}.
- 将实验结果与使用时间依赖密度函数理论 (TD-DFT) 的理论计算进行比较.
- 为了研究连接物交换对纳米集群光学性质的影响.
主要方法:
- 光学吸收光谱在一个广泛的能量范围 (0.056.2 eV).
- 净化纳米集群样本用于固体和溶液相位测量.
- 在线性响应模式中使用TD-DFT进行理论计算.
- 与谷氨的连接物交换实验.
主要成果:
- 在NIR-vis区域的实验和计算的摩尔吸收系数在2的系数内达成一致.
- 在1.53.5 eV之间观察到特有的吸收特征.
- 电子转换的开始被实验确定为0.45 ± 0.05 eV,与计算的0.55 eV非常接近.
- 带振动有助于在电子过渡下面的红外特征.
- 对谷氨的部分连接体交换并没有改变电子过渡的开始.
结论:
- 这项研究提供了AU102) p-MBA) p44) 纳米集群的全面光谱表征.
- 实验和理论光学吸收数据显示良好一致.
- 金属核心的电子特性对连接物交换具有坚固性,表明稳定性.
- 这些发现可以作为对纳米集群操纵和应用的未来研究的基准.
更多相关视频
相关概念视频
¹H NMR: Complex Splitting
A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
UV–Vis Spectroscopy: Molecular Electronic Transitions
In Ultraviolet–Visible (UV–Vis) spectroscopy, the absorption of electromagnetic radiation is used to probe the electronic structure of molecules. This technique provides insights into molecular electronic transitions, particularly the movement of electrons between different molecular orbitals. Radiation is absorbed if the energy of the electromagnetic radiation passing through the molecule is precisely equal to the energy difference between the excited and ground states. During this process,...
Electronic Structure of Atoms
An atom comprises protons and neutrons, which are contained inside the dense, central core called the nucleus, with electrons present around the nucleus. Taking into account the wave–particle duality of electrons and the uncertainty in position around the nucleus, quantum mechanics provides a more accurate model for the atomic structure. It describes atomic orbitals as the regions around the nucleus where electrons of discrete energy exist, characterized by four quantum numbers: n, l, ml, and...
¹H NMR: Interpreting Distorted and Overlapping Signals
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
π Electron Effects on Chemical Shift: Overview
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0, resulting in...
¹H NMR Signal Multiplicity: Splitting Patterns
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...


