The competitive through-space and through-bond interaction of two symmetry-equivalent, semi-localized orbitals 'Pa, 'Pb (= 7T or lone-pair orbitals) in a molecule M of C s or higher symmetry can lead either to the natural order of the corresponding de localized orbitals, i.e., IjJ _ ':::::-('Pa -'Pb)/.j2 above 1jJ+ ' :::::-('Pa + 'Pb)/.,jI, or to the inverted order, i.e., IjJ + above IjJ _. It is shown that one can discriminate between these two situations through an analysis of the PE spectrum of a molecule M' which differs from M only by an additional semi-localized orbital 'Pc of known symmetry behaviour. The method is exemplified by an investigation of the dependence of the 7T-orbital sequence in 3,6-bridged 1,4cyclohexadienes on the dihedral angle between the two C-CH=CH-C moieties.Photoejection of an electron e" from a neutral, closed shell molecule M leads, according toto a radical cation M+ in the electronic state 'l1J =(1/10)2 (1/1,)2 (1/12)2 •.• (1/1 J)' ... (I/IN)2. This state belongs to the same symmetry species ( = irreducible representation) of the symmetry group of M as the vacated orbital 1/1J = };IlCJIleJ>W The current interest in molecular oribtals as qualitative (or semi-quantitative) model concepts for the rationalisation and prediction of chemical properties (e.g., [2]) has had a strong influence on the rapid development of photo-electron spectroscopy ( =PE spectroscopy). The reason is that this technique [3] yields information about orbital characteristics which are otherwise difficult, if not impossible, to obtain. Typical examples are a) orbital energies eJ = e(1/1 J ), which can be measured under the implicit assumption of the validity of Koopmans' theorem [4] , b) the relative locations of the nodes in the vacated orbital 1/ 1 J, which can be inferred in some cases from an analysis of the vibrational pattern of the corresponding PE bands [3,5],or c) the absolute value IcJp I of the coefficient of an atomic p orbital eJ>p centered at a heavy atom, which can be determined under favorable conditions (e.g., linear molecule * Part 33 of: Applications of photoelectron-spectroscopy; for part 32, see Ref. I. 143 144 E. HEILBRONNER lsr. J. Chem.,