Abstract:We report a detailed calculation of total elastic, differential elastic, momentum transfer and electronic excitation for electron impact on difluoroacetylene (C2F2) molecules using the R-matrix method at low energies. After testing many target models, the final results are reported for the target model that gave the best target properties and predicted the lowest value of the shape resonance. The shape resonance is detected at 5.86 eV and 6.49 eV with the close-coupling and static exchange models due to 2Πg (2… Show more
“…This section discusses the recent results obtained by Gupta et al for C 2 F 2 [60], C 3 F 4 [61], and C 4 F 6 isomers [62] for elastic and inelastic scattering at low energies and C 2 F 6 [34] for ionization. Figure 1(a) shows the application of the R-matrix and SCOP methods at low, intermediate, and high energies to calculate the elastic cross section, as studied by Gupta et al [60]. The result is shown for C 2 F 2 .…”
Section: Resultsmentioning
confidence: 93%
“…The shifting of resonances to higher energies may be due to the shortening of the C-C bond in the case of C 2 F 2 and C 3 F 4 compared to C 2 H 2 and C 3 H 4 . A detailed explanation for such behavior is given in our previous articles [60,61]. It should be noted that there are no experimental or theoretical data available for such small fluorocarbon species.…”
Section: Resultsmentioning
confidence: 97%
“…Moreover, the dis- Figure 1. (a) Elastic scattering cross section for e-C2F2 from low (0.1 eV) to high (5 keV) energies calculated using the R-matrix and spherical complex optical potential (SCOP) methods [60] and comparison with experimental data of Gauf et al for C2H2 [136]. (b) Elastic and total cross section for C3F4 [61] calculated using the R-matrix method and comparison with the experimental data of Szmytkowski et al for C3H4 [137].…”
Section: Resultsmentioning
confidence: 99%
“…The low and intermediate energies cross-section calculations for various collision processes for several fluorocarbons have been theoretically predicted [54 59]. In recent years, the scarcity of cross-section data for simple fluorocarbons has led to studies on the low-energy cross section of fluorocarbons, such as C 2 F 2 [60], C 3 F 4 [61], and C 4 F 6 isomers [62], for various elastic and inelastic processes using the R-matrix method. At intermediate and high energies, differential and total cross sections have been computed using the single-center approach for C 4 F 6 isomers [63].…”
A brief review of the electron collision studies of perfluorocarbons and SF 6 relevant to plasma is presented. The use of these gases in various applications of plasma is highlighted, and their possible replacement with gases that have a low global warming potential is suggested. The results for a few simple fluorocarbons are presented, i.e., C 2 F 2 , C 3 F 4 , and C 4 F 6 for elastic scattering and C 2 F 6 for ionization, and the requirement for further investigation is highlighted. This review is not extensive; however, it presents an important step towards understanding the lack of cross-section data for numerous fluorocarbon molecules/radical species. In addition, it highlights the requirement for the detailed study of fluoroketones and fluoronitriles, which are possible substitutes for SF 6 for various electron collisional processes other than ionization.
“…This section discusses the recent results obtained by Gupta et al for C 2 F 2 [60], C 3 F 4 [61], and C 4 F 6 isomers [62] for elastic and inelastic scattering at low energies and C 2 F 6 [34] for ionization. Figure 1(a) shows the application of the R-matrix and SCOP methods at low, intermediate, and high energies to calculate the elastic cross section, as studied by Gupta et al [60]. The result is shown for C 2 F 2 .…”
Section: Resultsmentioning
confidence: 93%
“…The shifting of resonances to higher energies may be due to the shortening of the C-C bond in the case of C 2 F 2 and C 3 F 4 compared to C 2 H 2 and C 3 H 4 . A detailed explanation for such behavior is given in our previous articles [60,61]. It should be noted that there are no experimental or theoretical data available for such small fluorocarbon species.…”
Section: Resultsmentioning
confidence: 97%
“…Moreover, the dis- Figure 1. (a) Elastic scattering cross section for e-C2F2 from low (0.1 eV) to high (5 keV) energies calculated using the R-matrix and spherical complex optical potential (SCOP) methods [60] and comparison with experimental data of Gauf et al for C2H2 [136]. (b) Elastic and total cross section for C3F4 [61] calculated using the R-matrix method and comparison with the experimental data of Szmytkowski et al for C3H4 [137].…”
Section: Resultsmentioning
confidence: 99%
“…The low and intermediate energies cross-section calculations for various collision processes for several fluorocarbons have been theoretically predicted [54 59]. In recent years, the scarcity of cross-section data for simple fluorocarbons has led to studies on the low-energy cross section of fluorocarbons, such as C 2 F 2 [60], C 3 F 4 [61], and C 4 F 6 isomers [62], for various elastic and inelastic processes using the R-matrix method. At intermediate and high energies, differential and total cross sections have been computed using the single-center approach for C 4 F 6 isomers [63].…”
A brief review of the electron collision studies of perfluorocarbons and SF 6 relevant to plasma is presented. The use of these gases in various applications of plasma is highlighted, and their possible replacement with gases that have a low global warming potential is suggested. The results for a few simple fluorocarbons are presented, i.e., C 2 F 2 , C 3 F 4 , and C 4 F 6 for elastic scattering and C 2 F 6 for ionization, and the requirement for further investigation is highlighted. This review is not extensive; however, it presents an important step towards understanding the lack of cross-section data for numerous fluorocarbon molecules/radical species. In addition, it highlights the requirement for the detailed study of fluoroketones and fluoronitriles, which are possible substitutes for SF 6 for various electron collisional processes other than ionization.
“…In the present work, we have used the spherical complex optical potential (SCOP) method to predict the elastic and MTCS at intermediate energies (up to 2000 eV). A detailed description of this method can be obtained from our previous articles [27,[48][49][50][51]. Here, we present an overview of the calculation.…”
The present article reports calculated elastic, differential, momentum transfer and excitation cross section for electron scattering from BF and BF 2 radicals using the ab-initio R-matrix method. The calculations are performed with complete active space -configuration interaction and static exchange models for both targets to yield scattering cross sections and resonance parameters. Elastic and momentum transfer cross sections are also calculated using the spherical complex optical potential method to cover a wide energy range. The total ionization cross section is also reported from ionization threshold to 5 keV. The calculated cross sections for these neutral species are important for BF 3 plasma and are reported for the first time to the best of our knowledge except ionization.
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