Recently we have predicted [Phys. Rev. Lett. May 2005] that Ti-decorated carbon nanotubes can absorb up to 8-wt% hydrogen at ambient conditions. Here we show that similar phenomena occurs in light transition-metal decorated C60. While Sc and Ti prefers the hexagon (H) sites with a binding energy of 2.1 eV, V and Cr prefers double-bond (D) sites with binding energies of 1.3 and 0.8 eV, respectively. Heavier metals such as Mn, Fe, and Co do not bond on C60. Once the metals are absorbed on C60, each can bind up to four hydrogen molecules with an average binding energy of 0.3-0.5 eV/H2. At high metal-coverage, we show that a C60 can accommodate six D-site and eight H-site metals, which can reversible absorb up to 56 H2 molecules, corresponding to 7.5 wt%.PACS numbers: 61.46.+w,84.60.Ve,81.07.De An efficient storage media for hydrogen is crucial for the advancement of hydrogen and fuel-cell technologies 1 . There have been a great number of reports on the search for new routes to engineer nanomaterials so that (a) they dissociate H 2 molecules into H atoms and (b) reversibly adsorb hydrogen molecules at ambient conditions 1,2,3,4,5,6,7,8,9 . Much effort has been focused on the engineering of carbon-based materials such as nanotubes 10,11 and metal hydrides such as alanates 12 . It is found that while hydrogen-carbon interaction is too weak 10 , the metal-hydrogen interaction is too strong for hydrogen storage at ambient conditions. Very recently we have shown 13 a novel way to overcome this difficulty by forming artificial metal-carbide like structures on carbon singled-wall nanotubes (SWNT). From accurate first-principles calculations, we show that a single Ti-atom adsorbed on a SWNT can strongly bind up to four hydrogen molecules 13 . At large Ti coverage we find that a (8,0) SWNT can store hydrogen molecules up to 8-wt%, exceeding the minimum requirement of 6-wt% for practical applications. Even though these results were totally unexpected, we explained them by a simple Dewar, Chatt, and Duncanson (DCD) model 14,15 , where the interaction is due to donation of charge from the highest occupied orbital of the ligand to the metal empty states and a subsequent back donation from filled d-orbitals into the lowest unoccupied orbital of the ligand.Here we show that similar phenomena also occurs in light-transition metal decorated C 60 molecules. Below we first discuss several possible absorption sites for a single Ti atom on a C 60 molecule. We then show how a single Ti atom on a C 60 can bind up to four hydrogen molecules via Kubas interaction 14,15 . Multiple metal coverage cases, yielding up to 8 wt% hydrogen absorption, are discussed next. Finally, we briefly discuss the results for other transition metals from Sc to Co.The energy calculations were performed within the plane-wave implementation 16 of the generalized gradient approximation 17 to DFT. We used Vanderbilt ultra- soft pseudopotentials 18 treating the following electronic states as valence: Ti: 3s 2 3p 6 3d 2 4s 2 , C: 2s 2 2p 2 and H: 1s. The cutoff e...