Ex parte HILL et al. - Page 5




          Appeal No. 1997-3512                                       Page 5           
          Application No. 08/482,034                                                  

          same.  The examiner argues (answer, pages 3 and 4) that the                 
          “p++” and “p” doping ranges of the two base layers define the               
          whole range of well known doping concentrations, and that any               
          point of doping concentration between these upper and lower                 
          bounds is therefore approximately the same doping                           
          concentration.                                                              
               From our review of Gaw, we are not in agreement with the               
          examiner’s characterization of the doping concentrations of                 
          Gaw’s base layers 12 and 13.  We find that Gaw does not                     
          reasonably suggest that the two layers have approximately the               
          same doping concentrations to the extent that they are both                 
          within the vicinity of lower and upper ranges of p and p++.                 
          To the contrary, Gaw is directed to a (page 2, col. 1, lines                
          6-9) “heterojunction bipolar transistor having a multilayer                 
          base structure, wherein the layer adjacent to the emitter is                
          more heavily doped than the layer adjacent to the collector.”               
          Base layer (13) is a “highly doped” p-type layer “p++” in                   
          contrast to base layer (12) which is a “lightly doped” p-type               
          layer “p.”  As further disclosed by Gaw (page 3, col. 4, lines              
          11-16), “It is believed that current flow is enhanced by the                
          presence of an accelerating field generated by the wide band                








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