Electronic relaxation dynamics in [Au 25 (SR) 18 ] −1 (R = CH 3 , C 2 H 5 , C 3 H 7 , MPA, PET) thiolate-protected nanoclusters
Electronic relaxation dynamics in [Au 25 (SR) 18 ] −1 (R = CH 3 , C 2 H 5 , C 3 H 7 , MPA, PET) thiolate-protected nanoclusters
复制标题
[Au 25 (SR) 18 ] â1 (R = CH 3 , C 2 H 5 , C 3 H 7 , MPA, PET) 硫醇盐保护的纳米团簇中的电子弛豫动力学
DOI:
10.1039/c9cp04039k
复制
发表时间:
2020
影响因子:
3.3
通讯作者:
Aikens, Christine M.
中科院分区:
文献类型:
--
作者:
Senanayake, Ravithree D.;Aikens, Christine M.
We investigate the excited electron dynamics in [Au25(SR)18]−1 (R = CH3, C2H5, C3H7, MPA, PET) [MPA = mercaptopropanoic acid, PET = phenylethylthiol] nanoparticles to understand how different ligands affect the excited state dynamics in this system. The population dynamics of the core and higher excited states lying in the energy range 0.00–2.20 eV are studied using a surface hopping method with decoherence correction in a real-time DFT approach. All of the ligated clusters follow a similar trend in decay for the core states (S1–S6). The observed time constants are on the picosecond time scale (2–19 ps), which agrees with the experimental time scale, and this study confirms that the time constants observed experimentally could originate from core-to-core transitions and not from core-to-semiring transitions. In the presence of higher excited states, R = H, CH3, C2H5, C3H7, and PET demonstrate similar relaxations trends whereas R = MPA shows slightly different relaxation of the core states due to a smaller gap between the LUMO+1 and LUMO+2 gap in its electronic structure. The S1 (HOMO → LUMO) state gives the slowest decay in all ligated clusters, while S7 has a relatively long decay. Furthermore, separate electron and hole relaxations were performed on the [Au25(SCH3)18]−1 nanocluster to understand how independent electron and hole relaxations contribute to the overall relaxation dynamics.