Metal hydrides are of considerable current interest, among other reasons, as potential hydrogen storage systems. 1,2 A design target of 6.5 wt % H has been regarded as adequate. We here report molecular-level calculations for a series of potential species of type MH 12 , where M is a group 6 atom, Cr, Mo, and W. They turned out to be stable as single molecules. In a hypothetical solid Li- (VH 12 ), the percentage would be 17, leaving plenty of room for adjustments. The isoelectronic ions VH 12 -, TiH 12 2-, and MnH 12 + also turned out to be stable. Our starting point was the Au/H chemical analogy [3][4][5][6] and the recent discovery of the icosahedral, 18-valence-electron species WAu 12 . 7-9 Its hydrogen analogues turned out to exist as stable minima but to have either a mixture of M-H and M(η 2 -H 2 ) bonds or only dihydrogen bonds. The literature on such bonds has been reviewed by Kubas 10 and Maseras et al. 11 The previous M-H n species had n values up to 9, occurring in ReH 9 2-. Thus, the new systems with n ) 12 would be a new record for metal hydrides. A single hydride ion in solid hydrogen is reported to form (H -)(H 2 ) 12 with n ) 24. 12 All species were studied using density functional theory, DFT, with the B3LYP exchange-correlation functional and second-order perturbation theory, MP2. For H, the 6-31g* basis set was used. For all metal atoms, energy-adjusted Stuttgart ECPs were used in order to take into account relativistic effects. 13 The number of valence electrons is 12 for Ti, 13 for V, 14 for Cr, Mo and W, and 15 for Mn. The 6s5p3d valence basis sets accompanying the ECPs were used 14 for all atoms. The calculations were repeated also with larger basis sets, in which the metal valence basis set were increased with one f function 6s5p3d1f. The H basis used in this second set of calculations was of the 6-31g** type, contracted to 2s1p. We shall report only the results obtained with the larger basis set. Equilibrium geometries and harmonic frequencies were computed for all species at the DFT level of theory and MP2 level of theory. To investigate the electronic structure of these species, some singlepoint energy calculations at the DFT-optimized geometries were repeated using the complete active space (CAS) SCF method 15 with dynamic correlation added by second-order perturbation theory (CASPT2). 16 The CASSCF/CASPT2 calculations were performed with all electron basis sets of the ANO type for all atoms. The exponents were optimized using the Douglas-Kroll Hamiltonian. The contracted basis set was 6s5p3d2f for Cr, 7s6p4d2f for Mo, 7s6p4d2f for W, and 2s1p for H. The active space included 12 active electrons in 12 active orbitals, which are the bonding and antibonding linear combination of the metal d orbitals and hydrogen s orbitals. Note that the four orbitals, mainly bonding to M np and ns AOs lie further down. The programs Gaussian03 and MOL-CAS6.0 17 were employed.We shall discuss first the neutral molecules and then the ionic species. All the MH 12 species were found to be local minima, wi...