There are many cases where energy is deposited by fast hadrons into a gaseous target consisting of a variety of components. Examples include, but are not restricted to, planetary atmospheres [1], reactor plasmas [2,3], liquid crystals [4], and intergalactic space [5]. In all of these systems, although they differ widely in density (n), the incoming projectile will deposit energy into some mixture of atoms, molecules, their ions, and electrons.To understand the energy deposition process, one needs to know the stopping power, or energy loss of the projectile with velocity v per unit track length: -dE (v)/dx. The stopping power of a substance is frequently normalized with regard to the density and referred to as the target cross section, S (v):In the simplest case, that of Bethe stopping [1], the stopping cross section of each component i can be written:Where Z 1 is the projectile charge and Z 2 is the target electron number. The stopping power of a target containing a mixture of components is then given, according to the Bragg rule [7] as a sum of the stopping powers of the target componentsIn terms of the stopping cross sections of the components, this becomes Thus, the mean excitation energy and thus the stopping cross sections of each of the components must be known.The stopping power and mean excitation energy of the electron gas is well known [8].Similarly, stopping powers and mean excitation energies of neutral atoms [9] and some molecules [10] are also well known, from theory or experiment, or both.The mean excitation energies of target ions and molecules, as would be expected in space and some plasmas, are much lesser known. In a recent paper [11], the mean excitation energies for all ions of some small atoms have been calculated using the aug-cc-pCV5Z basis set. Representative results for Ne are shown in the following Thus, information is available, or at least obtainable, for determination of the stopping properties of atoms, atomic ions, neutral molecules and electrons, so contribution to energy deposition by energetic hadrons in these systems can be determined. However, planetary atmospheres, deep space, and various plasmas contain polyatomic ions as well [5,[12][13][14]. . Thus, in order to understand the interaction of fast hadrons in space, the mean excitation energies of such ions must be available, and calculation of them is suggested here.