Ex parte GOLDENBERG - Page 10




          Appeal No. 96-2043                                                          
          Application 07/990,514                                                      


          larger, or 320 nsec.  This latter set of mirrors is arranged                
          so as to optically delay                                                    





          each of the 16 beams by time intervals )t  =rJ(r=0, 1, . . . ,              
                                                   r                                  
          15) so that these beams arrive at a common beam expander                    
          (convex                                                                     
          reflector) 25 in serial order, forming a temporally continuous              
          pulse (see FIG. 2) of time duration )t=16J.320 nsec.  The                   
          temporally sequenced pulses are reflected from the convex                   
          reflector 25 and expanded to fill the aperture of an amplifier              
          27.  After passage once through the amplifier, each pulse                   
          encounters a large concave reflector 29 that returns the pulse              
          through the amplifier for further amplification, and directs                
          it to a second convex reflector 31.   The reflector 31                      
          recollimates and directs each beam to an array 33 of plane                  
          100% reflectors, positioned in such a way that, after                       
          reflection from this array, the beams are parallel to each                  
          other, and all the pulses are temporally coincident.  The                   
          final pulse length is again 20 nsec.  See col. 3, line 50-col.              
                                         10                                           





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