ABSOLUTE CROSS-SECTIONS FOR DISSOCIATIVE ELECTRON-ATTACHMENT TO CONDENSED CH3CL AND CH3BR - EFFECTS OF POTENTIAL-ENERGY CURVE CROSSING AND CAPTURE PROBABILITY

Citation
P. Ayotte et al., ABSOLUTE CROSS-SECTIONS FOR DISSOCIATIVE ELECTRON-ATTACHMENT TO CONDENSED CH3CL AND CH3BR - EFFECTS OF POTENTIAL-ENERGY CURVE CROSSING AND CAPTURE PROBABILITY, The Journal of chemical physics, 106(2), 1997, pp. 749-760
Citations number
76
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
106
Issue
2
Year of publication
1997
Pages
749 - 760
Database
ISI
SICI code
0021-9606(1997)106:2<749:ACFDET>2.0.ZU;2-R
Abstract
We report cross sections for the trapping of 0-10 eV electrons by CH3C l and CH3Br physisorbed onto a Kr covered Pt substrate, measured as a function of Kr film thickness and methyl halide concentration. The mol ecules stabilize electrons incident at the surface by the dissociation of transient CH3Cl- and CH3Br- ions into an atomic anion and a neutra l fragment [dissociative electron attachment DEA]. For CH3Cl, the cond ensed phase absolute DEA cross section at approximate to 0.5 eV, reach es 13x10(-18) cm(2)+/-50%, which is 10(4)-10(6) times larger than the gas phase cross section, At higher energies (5-10 eV) for CH3Cl, our m easurements provide a lower limit for the DEA cross section. For CH3Br , the maximum DEA cross section occurs below the vacuum level; we meas ure an absolute magnitude of 3.0x10(-16) cm(2)+/-50% near 0 eV, which is 100 times larger than the corresponding gas phase value. These enha ncements in cross section arise from the lowering of the potential ene rgy surfaces of intermediate anions due to polarization induced in the Kr layer and metal substrate. An increase in DEA cross section with a reduction in the distance of transient anions from the metal surface, is explained by the effect of image charges on the energy at which an ion and neutral ground state potential energy curves cross. Below thic knesses of 5 ML of Kr, a decrease in DEA cross section is observed and attributed to a reduction in the electron capture probability of the halide due to competition with transfer to the metal substrate. (C) 19 97 American Institute of Physics.