Page 325 - DMTH402_COMPLEX_ANALYSIS_AND_DIFFERENTIAL_GEOMETRY
P. 325

Complex Analysis and Differential Geometry




                    Notes          Now, fix 1  k  2, and consider the over-determined system:

                                                                  u   k    a ,  i  1,2.
                                                                       k
                                                                   u i  i
                                   The  integrability  condition  for  this  system  is  exactly  (2),  hence  there  is  a  solution  in  a
                                                                                                           a
                                                                                        1
                                                                                                            k
                                   neighborhood of u . Furthermore, since the Jacobian of the map    u ,u 2   u ,u   1   2   is d    ,
                                                 0
                                                                                                            i
                                   and  det a k i  0,  it follows from the inverse function theorem, that perhaps on yet a smaller
                                           
                                   neighborhood,     is  a  diffeomorphism.  Let      1 ,   then    is  a  diffeomorphism  on  a
                                                                           ,
                                                                    
                                                   
                                   neighborhood V  of  (u ),  and if we set  X   X   then:
                                                                         
                                                      0
                                                0
                                                                       u
                                                                             j
                                                                
                                                                X   X j    u i j    X b   Y . i
                                                                             i
                                                                 i
                                                                            j
                                   Proposition 2. Let  X : U    be a parametric surface, and let Y  and Y  be linearly independent
                                                         3
                                                                                     1
                                                                                           2
                                   vector fields. Then for any point u   U there is a neighborhood of u  and a reparametrization
                                                                                          0
                                                              0
                                   
                                                   
                                                         
                                   X   X   such that  X  f Y  for some functions f . i
                                        
                                                       i
                                                        i
                                                    i
                                   Proof. By Lemma 1 is suffices to show that there are function f  such that f  Y  and f  Y  commute.
                                                                                    i
                                                                                             1
                                                                                                    2
                                                                                               1
                                                                                                      2
                                             
                                   Write Y ,Y   a Y  a Y ,  and compute:
                                                  1
                                                1
                                            2
                                          1
                                                       2
                                                     2
                                                    f Y ,f Y    f f  a Y  a Y   f   Y f Y     f   Y f Y .  
                                                     1  1  2  2  1 2  1  1  2  2  1  1 2  2  2  2 1  1
                                                     f Y ,f Y    vanishes if and only if the following two equations are satisfied:
                                   Thus, the commutator  1  1  2  2
                                                                   Y f  – a f  = 0
                                                                     2 1
                                                                          1 1
                                                                   Y f  – a f  = 0.
                                                                     1 2
                                                                         2 2
                                   We can rewrite those as:
                                                                   Y  log f  = a 1
                                                                     2
                                                                          1
                                                                   Y  log f  = a .
                                                                          2
                                                                             2
                                                                     1
                                   Each of those equation is a linear first-order partial differential equation, and can be solved for
                                   a positive solution in a neighborhood of u .
                                                                     0
                                   In a neighborhood of a non-umbilical point, the principal directions define two orthogonal unit
                                   vector fields. Thus, we obtain the following Theorem as a corollary to the above proposition.
                                   Theorem 1. Let  X : U    be a parametric surface, and let u  be a non-umbilical point. Then
                                                       3
                                                                                    0
                                                                                     
                                                                                                      
                                   there  is  neighborhood  U   of  u   and  a  diffeomorphism    : U   U   such  that  X  X    is
                                                                                                          
                                                                                           0
                                                                                      0
                                                             0
                                                        0
                                   parametrized by lines of curvature.
                                   If X is parametrized by lines of curvature, then the second fundamental form has the coordinate
                                   representation:
                                                                             0 
                                                                       1
                                                                 k
                                                                       k g 11  k g 22  
                                                                        0
                                                                  ij
                                                                             2
                                   Definition 2. A curve  on a parametric surface X is called an asymptotic line if it has zero normal
                                                    
                                                  , 
                                   curvature, i.e.,   k    0.
          318                               LOVELY PROFESSIONAL UNIVERSITY
   320   321   322   323   324   325   326   327   328   329   330