In the natural photosynthetic centers of bacteria and plants, antenna chromophores absorb solar light and transfer the excitation energy to the reaction center by highly efficient singlet–singlet energy transfer. Spatial organization of individual chromophores is key to such efficiency: chromophores need to be separated enough to minimize selfquenching without sacrificing the dipole–dipole couplingmediated energy transfer. In addition to its important role in photosynthesis, efficient transfer of energy from multiple chromophores to a single acceptor is of potential significance to solar cells, photocatalysts, optical sensors and light-emitting devices. For these reasons, there has been a great deal of interest in mimicking the natural light-harvesting process. A variety of scaffolds have been used including dendrimers, organogels, porphyrin arrays/assemblies, biopolymer assemblies, and organic–inorganic hybrid materials. Although impressive results have been obtained with the above scaffolds, the multistep synthesis of the complex architectures hampers their scale up and widespread application. Nature relies on a combination of covalent and noncovalent interactions to create the photosynthetic centers. Covalent structures possess excellent stability and noncovalent self-assembled constructs provide order and synthetic efficiency. Herein, we report a biomimetic approach to construct artificial light-harvesting systems. We combined two self-assembling strategies and covalent fixation to prepare a highly efficient antenna system from readily available building blocks. The entire synthesis was achieved by a one-pot reaction, and the product precipitated spontaneously out of the reaction mixture at the end of the reaction. The synthesis of the light-harvesting system is shown in Scheme 1, and is based on the recently reported method to cross-link surfactant micelles. Our model antenna chromophore is 9,10-bis(4-methylphenyl)anthracene (DPA), a compound with high fluorescence quantum yield (90%). Eosin Y disodium salt (EY) is the energy acceptor. Cationic surfactant, 4-(dodecyloxy)benzyltripropargylammonium bromide (1), forms micelles at concentrations of above 0.14 mm in water. Because the surface of the micelle is covered with a dense layer of alkynyl groups, 1,4-diazidobutane-2,3-diol (2) could easily capture the micelle by 1,3dipolar cycloaddition with a Cu catalyst. When 1 and 2 were used in a 1:1 ratio, the resulting surface-cross-linked micelles (SCMs) are water-soluble nanoparticles with numerous alkynes on the surface. Surface functionalization occurred readily upon addition of a THF solution of DPA–N3 (obtained from commercially available DPA by partial bromination and azidation, see the Supporting Information). After 18 hours at room temperature, the DPA-functionalized SCMs (DPA– SCMs) precipitated spontaneously from the 2:1 THF/water mixture, apparently as a result of the increased hydrophobicity of the product. The IR spectrum of the DPA–SCMs showed nearly complete disappearance of the alkyne peaks in the starting SCMs (Figure S1, in the Supporting Information). DLS (dynamic light scattering) indicated an increase in size for the SCMs upon DPA-functionalization (Figure S2, in the Supporting Information). The absorption band of the DPA–SCMs is at 330–420 nm in THF and the emission band at 390–520 nm. These spectra match almost exactly with those of the free, monomeric DPA in solution (Figure S3, in the Supporting Information). Therefore, the DPA concentration ([DPA]SCMs) in this system can be determined from the absorption spectrum and the molar coefficient extinction of DPA. A frequent issue in light-harvesting systems with multiple donors is the self-quenching and/or excimer formation caused by the proximity of the chromophores. These pathways interfere with the energy transfer and lower the overall efficiency, and often require elaborate strategies to overcome. Excitingly, the fluorescence quantum yield was 0.80 and 0.90 for the micelle-bound DPA and the free chromophore, respectively (see the Supporting Information). Clearly, neither self-quenching nor excimer formation was significant in the highly crowded system. We suspect there are [*] H.-Q. Peng, Dr. Y.-Z. Chen, Prof. Q.-Z. Yang, Prof. L.-Z. Wu, Prof. C.-H. Tung, Prof. L.-P. Zhang Key Laboratory of Photochemical Conversion and Optoelectronic Materials, Technical Institute of Physics and Chemistry Chinese Academy of Sciences 29 Zhongguancun East Road, Beijing 100190 (China) E-mail: qzyang@mail.ipc.ac.cn H.-Q. Peng, Prof. Q.-X. Tong Department of Chemistry, Shantou University Shantou, Guangdong 515063 (China) E-mail: qxtong@stu.edu.cn