Ex parte HEFFNER et al. - Page 6




              Appeal No. 1998-2473                                                                                       
              Application No. 08/556,890                                                                                 


              have not made them.  Arguments not made are waived.  In re Kroekel, 803 F.2d 705, 709,                     
              231USPQ 640, 642-643 (Fed. Cir. 1986).                                                                     
                     We now turn to the rejection of claims 1, 3 and 6 based on Wilkinson.                               
                     Appellants argue that Wilkinson’s detector does not measure the power of the                        
              signal at the dither frequency and does not move the lens to maximize that power.  In fact,                
              argue appellants, Wilkinson does not measure any quantity at the dither frequency.                         
              Appellants contend that the differences between the instant claimed invention and                          
              Wilkinson are more than a matter of design choice.  More specifically, appellants point out                
              that Wilkinson requires the surface whose position relative to the lens is being adjusted to               
              also be moving in a direction perpendicular to the light beam so as to generate a time-                    
              varying signal whereas the instant invention has no such limitation.  Also, according to                   
              appellants, Wilkinson can only provide adjustments perpendicular to the disk surface.                      
                     We do not agree with appellants as to their argument pertaining to Wilkinson                        
              providing adjustments only perpendicular to the surface since the instant claims have no                   
              such limitation, requiring movement only “along a first axis.”                                             
                     As to the arguments regarding Wilkinson’s failure to measure the power of the                       
              signal at the dither frequency and that Wilkinson does not move the lens to maximize                       






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