Ex Parte HAVEMANN - Page 15



          Appeal No. 2005-0287                                      Page 15           
          Application No. 09/216,214                                                  

          device size can be minimized.4  See, e.g., the abstract, column             
          1, lines 50-60, column 2, lines 3-8 and column 6, line 44 through           
          column 7, line 24 of Watabe.  That disclosure of Watabe is                  
          consistent with the  examiner’s stated rationale for combining              
          the applied references, as referred to above.  That rationale for           
          the examiner’s rejection has not been specifically refuted by               
          appellant in the briefs before us in this appeal.5                          


               4 Appellant appears to be concerned with the same problem.             
          As set forth at the paragraph bridging pages 2 and 3 of                     
          appellant’s specification:                                                  
                    One of the long-standing problems in small field                  
               effect transistors is hot carrier effects. When a                      
               conventional MOS transistor structure is scaled down to                
               one micron or less, the potential energy of an electron                
               changes dramatically when it hits the N+ drain                         
               boundaries. This sudden change in potential energy in a                
               short distance creates a high electric field. This is                  
               undesirable because it causes the electrons to behave                  
               differently within the semiconductor lattice. Electrons                
               which have been activated by high electric fields are                  
               referred to as ‘hot electrons’, and can, for example,                  
               penetrate into or through the gate dielectric.                         
               Electrons which penetrate into, but not through, the                   
               gate dielectric can cause the gate dielectrics to                      
               become charged up over time. Thus, the behavior of the                 
               transistor will gradually shift in the field, until the                
               transistor may fail in service. This is extremely                      
               undesirable.                                                           
               5 We note that arguments not made in the briefs are not                
          generally considered by the Board.  See 37 CFR 1.192(a), as in              
          effect at the time the briefs were filed.  That regulation has              
          recently been replaced.  See 37 CFR 41.37(c)(vii).                          





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