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Complex Analysis and Differential Geometry




                    Notes          Then by cor. to Cauchy’s Theorem, we have

                                                       n
                                               f(z) dz  =   f(z) dz                                       (4)
                                              C        r 1  r 
                                                       
                                   Now, if a  is a pole of order m, then by Laurent’s theorem, f(z) can be expressed as
                                          r
                                                            m   b
                                                  f(z) = (z) +   s
                                                            s 1 (z a )  r  s
                                                            
                                   where (z) is regular within and on  .
                                                                r
                                          Then
                                                           m    b
                                                   f(z) dz  =     s  s  dz
                                                            
                                                  r       s 1 (z a )  r
                                                             r
                                                  (5)
                                   where     f(z) dz  0,  by Cauchy’s theorem
                                          r
                                   Now, on   |z-a | =  i.e. z = a  + e i
                                                           r
                                               r
                                           r
                                                dz =  ie  d
                                                        i
                                   where  varies from 0 to 2 as the point z moves once round g . r
                                                    m       2
                                   Thus,   f(z) dz  =   b   1-s  0   e (1 s)i  id
                                                               
                                                      s
                                                    
                                                  s 1
                                           r
                                          = 2pi b 1
                                          = 2pi [Residue of f(z) at a ]
                                                              r
                                                      
                                   where   0   2 e (1 s)i  d  =   0, if s  1 1
                                               
                                                       2 if s 
                                                        
                                                      
                                   Hence, from (4), we find
                                                   n
                                           f(z)dz  =   2 i [Residue of f(z) at a ]
                                                      
                                                                       r
                                          C        r 1
                                                   
                                                        n
                                                     = 2i    Residue of f(z) at a r  
                                                        r 1              
                                                        
                                                     = 2i [sum of Residues of f(z) at its poles inside C.]
                                   which proves the theorem.


                                   Remark. If f(z) can be expressed in the form f(z) =    (z)   where (z) is analytic and (a)  0, then
                                                                          (z a) m
                                                                            
                                   the pole z = a is a pole of type I or overt.
                                   If f(z) is of the form f(z) =    (z) ,  where (z) and (z) are analytic and (a)  0 and (z) has a zero
                                                        (z)
                                   of order m at z = a, then z = a is a pole of type II or covert. Actually, whether a pole of f(z) is overt
                                   or covert, is a matter of how f(z) is written.



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