Size-dependent luminescence is one of the most promising properties in semiconductor nanocrystals.1 -3 Such sizedependent luminescence is also found in various metal nanocrystals like the gold nanoclusters.4 -6 For example, blue luminescence was observed from Au 8 , which was stabilized and encapsulated by dendrimers. The color of the luminescence was extended to near-IR, as the size of the gold nanoclusters increased, 7,8 which was attributed to the confinement of the cluster sizes comparable to the Fermi wavelength of electrons (approximately 0.7 nm). 9 We recently studied the luminescence of the gold nanoclusters, especially the blue luminescence of Au 8 , 10 which provided a clue to the origin of luminescence in the gold nanoclusters. 11 -13 In this work, we examined the electronic transitions of Au 8 to elucidate the photoluminescence spectrum of the gold nanoclusters in more detail. The calculated geometries and energies of the isomers in Au 8 indicated that one isomer was more stable than the others, implying that a single isomer was the main contributor to the photoluminescence spectrum of Au 8 . The calculated spectrum of the most stable isomer agreed with the experimental spectrum, suggesting that several excited states of the single isomer contributed to the photoluminescence spectrum, whose shape was broad and asymmetric.The photoluminescence of the gold nanoclusters encapsulated by dendrimers was previously reported. 10 The emission maximum at 460 nm (2.7 eV) matched the emission energy of Au 8 (2.75 eV) in the spherical jellium approximation (Figure 1 (a)).8 On the other hand, the photoluminescence band was broad and asymmetric, which was ascribed to the spectral overlapping of emission bands.10 Indeed, the photoluminescence spectrum could be deconvoluted by two Gaussian functions. The low-energy band at 535 nm (2.32 eV) happened to agree with the emission energy of Au 13 (2.34 eV) in the spherical jellium model. 8 In this regard, another nanocluster was previously assigned as Au 13 , 10 because Au 13 was also the stable size of the gold nanoclusters. 8 For better understanding of the broad and asymmetric shape, the electronic transitions of Au 8 were calculated using the GAUSSIAN program.14 At first, the stable geometries and energies of Au 8 were obtained, by analytical gradients with full optimization using ab initio method such as the Møller-Plesset perturbation theory (MP2) and the density functional theory (DFT) such as Becke three-parameter Lee-Yang-Parr (B3LYP) and Perdew-Wang 1991 (B3PW91) gradient corrected exchange and correlation functional at two basis sets (CEP-4G and LANL2DZ). These levels of calculation have been frequently employed to obtain the stable geometries and energies of small gold nanoclusters. 15 -17 Since the emission energy of the dendrimer-encapsulated Au 8 matched the spherical jellium model, three-dimensional geometries were mainly examined, although the most stable geometry was known to be two-dimensional in the gas phase.15 -17 Among the optimized three-dimensio...