Ex Parte YAMADA - Page 10




          Appeal No. 2000-1608                                                         
          Application 08/953,998                                                       

          has not been attempted by the Examiner even though claim 1 is not            
          that complicated.  Appellant argues that the Examiner has used               
          language and made findings that are more appropriate to an                   
          obviousness rejection (Br7).  In response, the Examiner has spent            
          considerable time and effort discussing the arguments in                     
          Appellant's brief.  General discussions of Monte Carlo techniques            
          and what was known in the art are of no help to us in addressing             
          the specifics of claim 1.  Therefore, we make our own findings               
          regarding the anticipation rejection over Yamada.                            
               We find that Yamada is essentially directed to the admitted             
          prior art of Appellant's Fig. 1, wherein ejection angle                      
          distribution values calculated using MD techniques are used to               
          calculate atom trajectories using the MC method.  Yamada does not            
          teach the second, third, fourth, and fifth steps of claim 1.                 
               The characteristic feature of Appellant's invention is                  
          calculating (in a particular way) a continuous vertical                      
          distribution function from a calculated direction-dependent                  
          distribution of ejected particles (second step).  Then the                   
          distribution function is used to determine a value of the                    
          vertical angle 2 likely to emerge in a random process of a                   
          particle ejection (third step) and a value of a horizontal                   
          angle N likely to emerge in a random process of a particle                   
          ejection is determined (fourth step).  Last is the step of                   


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