KINETICS OF FIELD EVAPORATION OF GALLIUM PHOSPHIDE IN THE PRESENCE OF HYDROGEN

1989 ◽  
Vol 50 (C8) ◽  
pp. C8-141-C8-146
Author(s):  
A. GAUSSMANN ◽  
W. DRACHSEL ◽  
J. H. BLOCK
Keyword(s):  
Gallium Phosphide ◽  
Field Evaporation ◽  
Kinetics Of

Experiments on the kinetics of field evaporation of small ions from droplets

1995 ◽  
Vol 103 (12) ◽  
pp. 5041-5060 ◽  
Author(s):  
I. G. Loscertales ◽  
J. Fernández de la Mora
Keyword(s):  
Field Evaporation ◽  
Kinetics Of

Kinetics of field evaporation during hydride formation on GaP surfaces: a FIM and atom-probe study

Langmuir ◽  
1992 ◽  
Vol 8 (1) ◽  
pp. 125-129 ◽  
Author(s):  
A. Gaussmann ◽  
W. Drachsel ◽  
J. H. Block
Keyword(s):  
Atom Probe ◽  
Field Evaporation ◽  
Hydride Formation ◽  
Kinetics Of

Kinetics of Silicon field evaporation

2018 ◽  
Vol 146 ◽  
pp. 319-323
Author(s):  
Markus Karahka ◽  
H.J. Kreuzer
Keyword(s):  
Field Evaporation ◽  
Kinetics Of

Direct observations of radiation-enhanced transformations in glass

1983 ◽  
Vol 41 ◽  
pp. 354-355
Author(s):  
J. F. DeNatale ◽  
D. G. Howitt
Keyword(s):  
Glass Matrix ◽  
Diffusion Mechanism ◽  
Bubble Formation ◽  
Silicate Glasses ◽  
Phase Decomposition ◽  
Direct Observations ◽  
Thin Foils ◽  
Oxygen Bubble ◽  
Electron Energy Loss ◽  
Kinetics Of

The electron irradiation of silicate glasses containing metal cations produces various types of phase separation and decomposition which includes oxygen bubble formation at intermediate temperatures figure I. The kinetics of bubble formation are too rapid to be accounted for by oxygen diffusion but the behavior is consistent with a cation diffusion mechanism if the amount of oxygen in the bubble is not significantly different from that in the same volume of silicate glass. The formation of oxygen bubbles is often accompanied by precipitation of crystalline phases and/or amorphous phase decomposition in the regions between the bubbles and the detection of differences in oxygen concentration between the bubble and matrix by electron energy loss spectroscopy cannot be discerned (figure 2) even when the bubble occupies the majority of the foil depth.The oxygen bubbles are stable, even in the thin foils, months after irradiation and if van der Waals behavior of the interior gas is assumed an oxygen pressure of about 4000 atmospheres must be sustained for a 100 bubble if the surface tension with the glass matrix is to balance against it at intermediate temperatures.

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