Surface waves above thin porous layers and periodic structures

1999 ◽  
Vol 105 (2) ◽  
pp. 1385-1385 ◽  
Author(s):  
Walter Lauriks ◽  
Luc Kelders ◽  
Jean François Allard
1998 ◽  
Vol 104 (2) ◽  
pp. 882-889 ◽  
Author(s):  
Luc Kelders ◽  
Walter Lauriks ◽  
Jean F. Allard
Keyword(s):  

2004 ◽  
Vol 116 (3) ◽  
pp. 1345-1347 ◽  
Author(s):  
Jean F. Allard ◽  
Michel Henry ◽  
Vincent Gareton
Keyword(s):  

1988 ◽  
Vol 65 (7) ◽  
pp. 769-773
Author(s):  
L.A. Chernozatonskii ◽  
D.K. Gramotnev ◽  
V.I. Pustovoit

Author(s):  
Frances M. Ross ◽  
Peter C. Searson

Porous semiconductors represent a relatively new class of materials formed by the selective etching of a single or polycrystalline substrate. Although porous silicon has received considerable attention due to its novel optical properties1, porous layers can be formed in other semiconductors such as GaAs and GaP. These materials are characterised by very high surface area and by electrical, optical and chemical properties that may differ considerably from bulk. The properties depend on the pore morphology, which can be controlled by adjusting the processing conditions and the dopant concentration. A number of novel structures can be fabricated using selective etching. For example, self-supporting membranes can be made by growing pores through a wafer, films with modulated pore structure can be fabricated by varying the applied potential during growth, composite structures can be prepared by depositing a second phase into the pores and silicon-on-insulator structures can be formed by oxidising a buried porous layer. In all these applications the ability to grow nanostructures controllably is critical.


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