Semiconductor nanocrystals with adjustable hole acceptors: tuning the fluorescence intensity by metal-ion binding.
Semiconductor nanocrystals with adjustable hole acceptors: tuning the fluorescence intensity by metal-ion binding.
复制标题
DOI:
10.1002/anie.201001441
复制
发表时间:
2010-09
影响因子:
--
通讯作者:
Jessica Völker;Xiaoyin Zhou;Xuedan Ma;Sandra Flessau;Hengwei Lin;M. Schmittel;A. Mews
中科院分区:
文献类型:
--
作者:
Jessica Völker;Xiaoyin Zhou;Xuedan Ma;Sandra Flessau;Hengwei Lin;M. Schmittel;A. Mews
Semiconductor nanocrystals (NCs) are robust inorganic chromophores that combine an efficient broadband absorption with a narrow-band fluorescence spectrum. Hence, they have a great potential as photoactive systems in attractive applications such as biolabeling,[1] solar cells,[2, 3] light-emitting diodes,[4] and even in sensor systems.[5–7] Whereas most of these applications rely on the tunability of the fluorescence wavelength and thus on the size of the particles, sensor devices require a change of the fluorescence intensity, which strongly depends on surface effects in NCs. As the fluorescence arises from the recombination of photoexcited electron–hole pairs (excitons) within the inorganic NC core, its intensity is lowered if charge carriers are transferred to surface-bound ligands. This process, involving a photoinduced electron transfer (PET), strongly depends on the energetic position of the electronic levels of the NC with respect to those of the molecular orbitals (MOs) of the ligands. It has been known for many years that ligands may either increase or decrease the fluorescence intensity of NCs. For example, for the well-known CdSe NCs, prepared by standard methods in trioctylphosphine oxide (TOPO),[8] the replacement of TOPO ligands by amines increases the fluorescence intensity,[9] whilst that by thiols leads to a complete fluorescence quenching.[10] For CdTe NCs, prepared by similar methods, the situation is reversed: ligand exchange of TOPO by thiols leads to an increase of the fluorescence intensity.[10] The fluorescence quenching is assumed to be due to a transfer of the photoexcited hole from the top of the NC valence band (VB) to the highest occupied molecular orbital (HOMO) of the attached ligand.[10]