Directional emission of nonthermal halogen atoms by electron bombardment of alkali halides

1989 ◽  
Vol 39 (17) ◽  
pp. 12950-12953 ◽  
Author(s):  
Z. Postawa ◽  
M. Szymoński
1975 ◽  
Vol 35 (20) ◽  
pp. 1382-1385 ◽  
Author(s):  
Ansgar Schmid ◽  
Peter Bräunlich ◽  
Pieter K. Rol

1986 ◽  
Vol 75 ◽  
Author(s):  
R. E. Walkup ◽  
Ph. Avouris ◽  
A. P. Ghosh

AbstractWe present experimental results which suggest a new mechanism for the production of excited atoms and ions by electron bombardment of alkali-halides. Doppler shift measurements show that the electronically excited atoms have a thermal velocity distribution in equilibrium with the surface temperature. Measurements of the absolute yield of excited atoms, the distribution of population among the excited states, and the dependence of yield on incident electron current support a model in which excited atoms are produced by gas-phase collisions between desorbed ground-state atoms and secondary electrons. Similarly, gas-phase ionization of ground-state neutrals by secondary electrons accounts for a substantial portion of the positive ions produced by electron bombardment of alkali-halides.


The He I photoelectron spectra of the chlorides, bromides and iodides of Na, K, Rb and Cs have been recorded in the vapour state by a molecular beam technique. The spectra exhibit features which have been interpreted on the basis of a completely ionic model in keeping with the treatments usually applied to ionic solids. To explain structure in the spectra of the lighter molecules it has been necessary to discuss polarization of the halogen atoms by the alkali metal ions. For the heavier molecules such as KI, RbI and Csl the spectra of the monomers consist of two fairly broad bands corresponding to ionization of the X­­­­ˉmoiety to its 2 P 3/2 and 2 P ½ states. These have a 2/1 intensity ratio and a separation equal to 3/2 times the appropriate spin-orbit coupling coefficient. In the case of NaI the 2 P 3/2 state is split by the strong electrostatic field of the Na + ion into states possessing 2 ∏ 3/2 and 2 ∏ ½ character. This is accompanied by a shift of the 2 P ½ state to higher energies as it gradually assumes 2 ∑ character. The result is an increase of the mean 2 P 3/2 – 2 P ½ separation to a value greater than that to be expected from spin-orbit coupling alone. This increase becomes more pronounced for the bromides and chlorides where the spin-orbit coupling coefficient is smaller. For NaCl the separation of the 2 P 3/2 and 2 P ½ bands shows clearly that the 2 P½ band possesses considerable 2 ∑ character. In terms of partial ionic character, increased polarization of the halogen atom is related to increased covalent character of the MX bond. The lighter molecules can therefore be said to be the least ionic in this description. The proportion of dimers to monomers observed in the spectra is found to fall as the molecules become more ionic, i. e. as the halogen atoms become less polarized.


1986 ◽  
Vol 57 (17) ◽  
pp. 2227-2230 ◽  
Author(s):  
R. E. Walkup ◽  
Ph. Avouris ◽  
A. P. Ghosh

1951 ◽  
Vol 29 (2) ◽  
pp. 122-128 ◽  
Author(s):  
D. E. McLennan

Electron bombardment experiments have been carried out on small crystals of the alkali halides within the electron microscope. Crystals of two size ranges were bombarded at high intensity, and evidence of a generalized photographic effect within the ionic group of solids is presented. The first group of crystal specimens ranged in size from 0.2 to 0.002 cm., the bombardment causing the formation of F-centers and entrapped metal colloids in the crystal lattice. Ionization pulses were observed to occur in the region of the specimen during bombardment. The second group ranged in size from 10 to 0.01 μ, observations on the effects of bombardment being carried out with electron diffraction techniques. A process has been suggested to explain the phenomenon of ionic crystals which appear to lose their centers under high electron beam intensity in the electron microscope.


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