ABSTRACrUsing the SCF-Xa-SW method the ground state electronic structures of (HO)3Mo==Mo(0H)3, (H2N) (7,8) and W2X6 (9-11) compounds. In these compounds there is a 3-fold axis of symmetry which makes it easy to formulate a qualitative, approximate description of the bonding. We have previously proposed a view in which one a and two Xr bonds formed mainly by metal d orbitals constitute the triple bond (8), but a valence-bond description in terms of three equivalent bent bonds is, at least in qualitative terms, also useful (12).To gain a better understanding of these triple bonds, and their relationship to the other electrons in the molecule, a quantitative treatment was desired, and in view of the proven effectiveness of the SCF-Xa-SW method of calculation (13) in dealing with related species containing quadruple bonds between metal atoms in the second transition series (14-16) this approach was adopted. In addition, since the volatility of the substances we are concerned with is high,' we have been able to test our calculations against the observed photoelectron spectra.Two types of compounds were selected for these first studies: Mo2(0R)6 and Mo2(NR2)& Experimental photoelectron spectra were recorded for Mo2(OR)6 in which R is (CH3)3CCH2, since this is the only compound of its type for which a structurally characterized dinuclear molecule is available (17); with-smaller R'groups, polymerization occurs via bridging oxygen atoms.The costs of publication of this article were defrayed in part by the payment of page charges from funds made available to support the research which is the subject of the article. This article must therefore be hereby marked "advertisement" in accordance with 18 U. S. C. §1734 solely to indicate this fact.
3109For the Mo2(NR2)6 type compound, experimental data on the structure (8) and photoelectron spectrum are those for R = CH3.Calculations were made first for the hypothetical molecules in which R = H. This was done in the interest of simplicity and economy. The replacement of more inductwe R groups, CH3and (CH3)3CCH2, by H may be expecqd to have little effect on the relative energies of the highest occupied orbitals. From general principles and previous knowledge of the photoelectron spectra of Mo2(O2CR)4 compounds (18,19) the absolute ionization energies would be expected to shift more or less uniformly by about 1 eV to lower values upon replacing H by CH3 or (CH3)3CCH2. In testing the calculated spectra against experiment, therefore, the necessity of such uniform shifts of all peaks in a given spectrum may be anticipated and the validity of the calculated spectra judged by how well the calculated and observed patterns match. In view of the complex pattern of higher filled orbitals found in the amido compound, we have also performed a ground state calculation for the Mo2(NMe2)6 molecule itself.
PROCEDURESCompounds were prepared and characterized as described elsewhere (8,17). He-I and He-TI photoelectron spectra were obtained using a Perkin-Elmer PS 16/18 photoelectron spectrometer f...