Ex parte BOMSE et al. - Page 12




         Appeal No. 1998-1814                                     Page 12          
         Application No. 08/347,814                                                


         lines 1-4, and col. 5, lines 13-16).  Demodulator 48 mixes the            
         detector signal with a signal at the second harmonic of the               
         laser modulation frequency, which is selected to be “between              
         500 Hz and ten kilohertz, 6.6 kilohertz being presently                   
         preferred” (col. 2, lines 5-9 and col. 4, line 68 through col.            
         5, line 1).  Mantz (‘273) similarly discloses (figure 1)                  
         parallel demodulation.  Amplifier 40 is used as a phase                   
         sensitive detector (col. 6, lines 55-68) for “locking the mid-            
         frequency of the cyclical laser scan to the absorption                    
         maximum.”  Mantz (‘273)further discloses (col. 4, lines 47-51)            
         that amplifier 40 is tuned to the frequency of laser 20, and              
         that amplifier 42, is preferably a tuned amplifier that is                
         tuned to twice the frequency of amplifier 40.  Mantz (‘273)               
         additionally discloses (col. 7, lines 12-15) that if amplifier            
         42 is a tuned phase-locked amplifier, the advantages of                   
         synchronous detection (i.e., noise and background suppression)            
         may be realized.                                                          
              From these teachings, we conclude that Mantz (‘448) and              
         Mantz (‘273) teach the limitations of claim 121.  Claim 155               
         contains language similar to claim 121.  We therefore affirm              
         the                                                                       







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