Electron-stimulated desorption of lithium atoms from oxygen-covered molybdenum surfaces

Citation
Vn. Ageev et al., Electron-stimulated desorption of lithium atoms from oxygen-covered molybdenum surfaces, SURF SCI, 451(1-3), 2000, pp. 153-159
Citations number
20
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
SURFACE SCIENCE
ISSN journal
00396028 → ACNP
Volume
451
Issue
1-3
Year of publication
2000
Pages
153 - 159
Database
ISI
SICI code
0039-6028(20000420)451:1-3<153:EDOLAF>2.0.ZU;2-P
Abstract
We have measured electron-stimulated desorption (ESD) yields and energy dis tributions for lithium (Li) atoms from Li layers adsorbed at 300 K on an ox ygen-monolayer-covered molybdenum surface as a function of electron energy and lithium coverage. The measurements have been carried out using a time-o f-flight method and surface ionization detector. The appearance threshold f or Li atoms is close to the O 2s level ionization energy of 25 eV and is in dependent of the lithium coverage. Above the 25 eV threshold the lithium at om ESD yield increases linearly with increasing lithium coverage. An additi onal threshold of 55 eV is observed in the lithium coverage range from O to 0.45; this appears to be associated with the Li Is level ionization energy . For energies above the 55 eV threshold the incremental change of lithium atom ESD yield exhibits a maximum as the lithium coverage increases, and de creases to zero at lithium coverages greater than 0.45. Additional features for lithium atoms appear at about 40 and 70 eV, correlating with the molyb denum 4p and 4s ionization energies at Li coverages of 0.6 and 0.75, respec tively. There are broad peaks at the latter energies indicating that desorp tion proceeds via a resonance process, in which the initial excitation may lead to a spectator electron in a quasi-bound state. The average kinetic en ergy of lithium atoms is several tenths of eV, It depends on the lithium co verage and electron energy. The ESD energy distribution for lithium atoms c onsists of a single peak with a maximum of around 0.18 eV for electron ener gies less than 55 eV. A second peak with a maximum of about 0.25 eV appears at electron energies greater than 55 eV. The data can be interpreted in te rms of the Auger-stimulated desorption model, in which neutralization of ad sorbed lithium ions occurs after filling of holes created by incident elect rons in inner shells of substrate and lithium atoms. (C) 2000 Elsevier Scie nce B.V. All rights reserved.