Abstract:We report measurements of differential and integral cross sections for electron excitation of the Schumann–Runge continuum, longest band, and second band electronic states in molecular oxygen. The energy range of the present study is 15–200 eV, with the angular range of the differential cross section (DCS) measurements from 2 to 130°. A generalized oscillator strength analysis is then employed in order to derive integral cross sections (ICSs) from the corresponding DCSs, and these ICSs are compared with releva… Show more
“…Thus, the level of agreement seen in Fig. 5 is heartening, and consistent with what we have observed previously 46,[56][57][58][59][60][61] for other species when resonance (i.e., the decay of a temporary negative (anion) state into the channel in question) effects are not apparent and when strong Rydberg-valence interactions are absent. With respect to Fig.…”
Section: Resultssupporting
confidence: 76%
“…5, we find a truly remarkable level of accord between our experimental ICSs and those from the BE f-scaling technique, over the common energy range of comparison. Benzene is by far the largest molecule we have yet considered in our studies 46,[56][57][58][59][60][61] seeking to investigate the efficacy of the BE fscaling approach, in particular in relation to providing reliable data bases for the plasma modeling community. Thus, the level of agreement seen in Fig.…”
We report results from measurements for differential and integral cross sections of the unresolved 1B1u and 3E2g electronic states and the 1E1u electronic state in benzene. The energy range of this work was 10–200 eV, while the angular range of the differential cross sections was ∼3°–130°. To the best of our knowledge there are no other corresponding theoretical or experimental data against which we can compare the present results. A generalized oscillator strength analysis was applied to our 100 and 200 eV differential cross section data, for both the 1B1u and 1E1u states, with optical oscillator strengths being derived in each case. The respective optical oscillator strengths were found to be consistent with many, but not all, of the earlier theoretical and experimental determinations. Finally, we present theoretical integral cross sections for both the 1B1u and 1E1u electronic states, as calculated within the BEf-scaling formalism, and compare them against relevant results from our measurements. From that comparison, an integral cross section for the optically forbidden 3E2g state is also derived.
“…Thus, the level of agreement seen in Fig. 5 is heartening, and consistent with what we have observed previously 46,[56][57][58][59][60][61] for other species when resonance (i.e., the decay of a temporary negative (anion) state into the channel in question) effects are not apparent and when strong Rydberg-valence interactions are absent. With respect to Fig.…”
Section: Resultssupporting
confidence: 76%
“…5, we find a truly remarkable level of accord between our experimental ICSs and those from the BE f-scaling technique, over the common energy range of comparison. Benzene is by far the largest molecule we have yet considered in our studies 46,[56][57][58][59][60][61] seeking to investigate the efficacy of the BE fscaling approach, in particular in relation to providing reliable data bases for the plasma modeling community. Thus, the level of agreement seen in Fig.…”
We report results from measurements for differential and integral cross sections of the unresolved 1B1u and 3E2g electronic states and the 1E1u electronic state in benzene. The energy range of this work was 10–200 eV, while the angular range of the differential cross sections was ∼3°–130°. To the best of our knowledge there are no other corresponding theoretical or experimental data against which we can compare the present results. A generalized oscillator strength analysis was applied to our 100 and 200 eV differential cross section data, for both the 1B1u and 1E1u states, with optical oscillator strengths being derived in each case. The respective optical oscillator strengths were found to be consistent with many, but not all, of the earlier theoretical and experimental determinations. Finally, we present theoretical integral cross sections for both the 1B1u and 1E1u electronic states, as calculated within the BEf-scaling formalism, and compare them against relevant results from our measurements. From that comparison, an integral cross section for the optically forbidden 3E2g state is also derived.
“…However, as observed in the high-resolution photoabsorption spectrum, the 1 Σ + state is overlapped with other vibrational progression as well as with the Rydberg-valence state of sσ with which the BE f -scaling approach may has its own limits of applicability, as is found in the longest band of O 2 . 39 Furthermore, the contribution of strong Rydberg-valence mixing affecting the 1 Π state may certainly be a general limitation in the BE f -scaling approach. These verifications await further investigations, both experimental and theoretical in the intermediate energy region below 60 eV.…”
The electronic state spectroscopy of carbonyl sulphide, COS, has been investigated using high resolution vacuum ultraviolet photoabsorption spectroscopy and electron energy loss spectroscopy in the energy range of 4.0–10.8 eV. The spectrum reveals several new features not previously reported in the literature. Vibronic structure has been observed, notably in the low energy absorption dipole forbidden band assigned to the (4π←3π) (1Δ←1Σ+) transition, with a new weak transition assigned to (1Σ−←1Σ+) reported here for the first time. The absolute optical oscillator strengths are determined for ground state to 1Σ+ and 1Π transitions. Based on our recent measurements of differential cross sections for the optically allowed (1Σ+ and 1Π) transitions of COS by electron impact, the optical oscillator strength f0 value and integral cross sections (ICSs) are derived by applying a generalized oscillator strength analysis. Subsequently, ICSs predicted by the scaling are confirmed down to 60 eV in the intermediate energy region. The measured absolute photoabsorption cross sections have been used to calculate the photolysis lifetime of carbonyl sulphide in the upper stratosphere (20–50 km).
“…Nonetheless, we caution that the Born approximation is not a very sophisticated approach and that as a result of this scaling procedures are often employed in conjunction with its use. 33,34 …”
Section: A Low Energies and Low Fields (0 E/n 0 35 Td) -The Need Formentioning
This paper revisits the issues surrounding computation of electron transport properties in water vapour as a function of E/n0 (the ratio of the applied electric field to the water vapour number density) up to 1200 Td. We solve the Boltzmann equation using an improved version of the code of Ness and Robson [Phys. Rev. A 38, 1446 (1988)], facilitating the calculation of transport coefficients to a considerably higher degree of accuracy. This allows a correspondingly more discriminating test of the various electron–water vapour cross section sets proposed by a number of authors, which has become an important issue as such sets are now being applied to study electron driven processes in atmospheric phenomena [P. Thorn, L. Campbell, and M. Brunger, PMC Physics B 2, 1 (2009)] and in modeling charged particle tracks in matter [A. Munoz, F. Blanco, G. Garcia, P. A. Thorn, M. J. Brunger, J. P. Sullivan, and S. J. Buckman, Int. J. Mass Spectrom. 277, 175 (2008)].
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