Atomic data for controlled fusion research

Abstract

22. Cross S :tiona for Formation of H Atoms in High Excited States by H* Impact on la, 1%, K, and Cm .... A.2.U 23. Excitation Cross Sections for the Reactions V Eg** H 2-H(2«,3s f 2p,3p,3<l) +H* • H 2 A.2.U6 i» 2k. Excitation Cross Sections for the Reactions H 2 * • H 2 * H 2 * • H • H(2s,2p,3p) il 2 * • H 2 * H 2 * • H • H(n « 3 • 2) A.2.U8 25. Excitation Cross Sections for the Reactions %•-H* • H° A.3.6 k. Dissociation Cross Sections for the Formation of Protons for B^* in He and the Formation of Past H° Atoms for H2* in H 2 A.3.8 5. Dissociation Cross Sections for the Formation of Protons for Ife* in I 2 and Re A.3.10 ¥ 6. Cross Sections for the Production Protons and H Atone for A^ in Mg and Ni A.3-12 7. Dissociation Cross Sections for the Production of Protons for the Reaction Products (H* + H°) for Ho* in Ar A.3.1 1 * 8. Cross Sections for the Ponation of Electronically Excited S *toms from the Dissociation of fio* and H 3 * fc» H 2 , •>, Hg, and Ha "". A.3-16 9. Dissociation Cross Sections for HD* Ions in He and 3e A.3.18 10. Dissociation Cross Sections for the Production of Past K* and Ho* fro* H 3 * in H 2 A.3.20 11. Dissociation Cross Sections for the Production of H° and H 2° fron H 3 * in H 2 A.3.22 12. Cross Sections for the Formation of Fast H* and H 2 * fron the Dissociation of H3+ in He and Re A.3.2U 13. Cross Sections for the Formation of H* H 2 + , and (H 2° • H°) fro« the Dissociation of H 3 * in Water Vapor A.3.26 Ik. Total and Partial Cross Sections for the Dissociation of HeH* in He A.3.28 1$. Total and Partial Cross Sections for the Dissociation of HeH* in Hg A.3.30 Continuations A.3.33 Electron Capture Cross Sections 1. Electron Capture Cross Sections for H~, H° and H* Passing Through Atonic Hydrogen A.U.2 2. Electron Capture Cross Sections for H* and H° Passing Through H 2 A.».» 3. Elactron Capture Cross Sections for H+ and H° Passing Through Helium A.U.6 U. Electron Capture Cross Sections for H* and H° Passing Through I 2 A.*.8 5. Electron Capture Cross Sections for H* and H° Passing Through 0 and Ofc A.U.10 6. Electron Capture Cross Sections for H* and H° Passing Through He Gas A.«.12 7. I .ectron Capture Cross Sections for H* and H° F using Through Ar A.U.iU <). Electron Capture Cross Sections for H* in H 2 0 and CHjj A.U.16 9. Electron Capture Cross Sections fbr H* in CO and CO2 Charges in H 2 and He by H* A.5. 1 * 3. Cross Sections for Production of Free Electrons in H2 end He by Protons A.5.6 k. Cross Sections for the Production of Slow H 2 and H* frosi H* and H c Impact on Hg A.5-8 5. Cross Sections for Positive Ion Production in M 2 and O2 by H* A.5-10 6. Cross Sections for Zlectron Production in »2 *nd 0 2 by H* A.5-12 T. Cross Sections for Production of n 2 * 9 S*, and H 2 * Ions by Protons in M 2 Gas A.5-1 1 * 8. Cross Sections for Production of O2*, 0* and 0 2 * Ions by Protons in Og A.5.16 9. Angular Distribution of Electrons from 300-keV Proton Impact in H 2 A.5.18 10. Angular Distribution of Electrons of Various Energies froa 300-keV Proton lapacts in H 2 A.5-20 11. Differ...

Strong Suppression of the Positronium Channel in Double Ionization of Noble Gases by Positron Impact

“…A third possible process [which is indistinguishable from (2) in our experiment] involves the formation of the positronium negative ion Ps 2 . Comparing to equivelocity proton data [2][3][4], the cross section for this double electron capture is expected to be very small, and it will not be considered further here.…”

Effect of energy chain branching in the hydrogen fiuorination reaction on the characteristics of an H2–F2laser

“…Sputtering yields were given by Sigmund [5]. These values are, however, several times higher than the experimental data for other heavy ions [6,7]; we have, therefore, divided Sigmund's sputtering yields by two for these calculations, S o . The energy and the angular distributions of sputtered impurity atoms were assumed to be:…”

Dynamic Light Scattering and Thermal Motion of Macromolecules in Solutions

“…The probability of an electron in group 1 colliding with a neutral before being lost is Figure 5 shows the total electron-neutral crosssections for molecular hydrogen and helium as well as the ionization cross-sections for various noble gases reproduced directly from Ref. [10]. Note that atomic cross-sections are very nearly the same for different isotopes.…”

“…5, and are taken directly from Ref. [10]. The most important parameter to determine in a specific device is |E_|.…”