Etching of Si through a thick condensed XeF2 layer
Author(s) -
P. G. M. Sebel,
L.J.F. Hermans,
H. C. W. Beijerinck
Publication year - 2000
Publication title -
journal of vacuum science and technology a vacuum surfaces and films
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.583
H-Index - 112
eISSN - 1520-8559
pISSN - 0734-2101
DOI - 10.1116/1.1288194
Subject(s) - etching (microfabrication) , sputtering , layer (electronics) , ion , silicon , materials science , yield (engineering) , reactive ion etching , ion beam , analytical chemistry (journal) , chemistry , optoelectronics , nanotechnology , composite material , thin film , organic chemistry , chromatography
Etching of silicon by XeF2 is studied in a multiple-beam setup. Below 150 K XeF2 condenses and forms a layer on the silicon, which blocks the etching. Upon ion bombardment, this layer is removed and etching will resume. As a function of the layer thickness, the various removal mechanisms of the layer are studied. For a thick condensed layer it is found that 1 keV Ar+ ions sputter the condensed layer with a yield of 160 XeF2 molecules per ion for 1 keV Ar+ ions and 280 for 2 keV ions. For thinner layers (below 9 nm for 1 keV ions), this sputter rate by ions decreases significantly. Here, the removal is mainly due to consumption of XeF2 by etching at the bottom of the layer. This consumption rate reaches a maximum for a layer thickness of about 5 nm. In the steady-state situation, the layer thickness is further decreased, resulting in a smaller consumption and etch rate. Here, sputtering is the most important removal mechanism for the deposited XeF2 layer. From this, it is concluded that a pulsed ion beam should be used in cryogenic etching to obtain the highest etch rate.
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