Ex parte SHINJI KOYANO et al. - Page 5




          Appeal No. 95-4372                                                         
          Application No. 08/043,610                                                 


                    The examiner reasoned that Kendall essentially disclosed         
          the claimed invention but for explicitly mentioning shifting the           
          phase of the receiver audio signal between ±120E and ±180E in the          
          mid- to high-frequency ranges.  The examiner then employed Tominari        
          as teaching this feature as well as a power amplifier and concluded,       
          somehow [see pages 10-11 of the principal answer], that the                
          combination of references would have resulted in the claimed subject       
          matter.  We disagree.                                                      
                    If the examiner is contending that it would have been            
          obvious to somehow use the phase shifter of Tominari in the system of      
          Kendall and then enclose the whole system in a single cabinet, we          
          find ourselves in agreement with appellants that Tominari teaches          
          away from employing a single cabinet.  Since Figure 7 and column 3,        
          lines 15-27 of Tominari indicate that the speakers therein should          
          generally oppose each other and not generate sound in the same             
          direction, this is a clear indication that the artisan would not have      
          sought to employ the speakers of Tominari in a "single cabinet."           
          Therefore, the question arises as to why the artisan, against the          
          teachings of Tominari, would have employed the phase shifter of            
          Tominari, used for generating a delay in order to give the feeling of      
          a concert hall and in an environment where the sounds from speakers        
          are not directed in the same direction, in the system of Kendall           

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