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Complex Analysis and Differential Geometry




                    Notes          Let  Y T U,  the covariant derivative of Z along Y is:
                                        
                                          u
                                                                          i
                                                                     Y Z   y Z .
                                                                            ;i
                                   We write the components of   Y Z  as:
                                                                           k
                                                                    j
                                                               z j  ;i   z   j ik z ,                  ...(10)
                                                                     ,i
                                               i
                                                 j
                                                   .
                                   so that   Y Z   y z   Furthermore, note that
                                                 ;i
                                                   j
                                                                     k
                                                                    k .                              ...(11)
                                                                 i
                                                                     ij
                                                                  j
                                   Our first task is to show that covariant differentiation is reparametrization invariant. However,
                                   since the metric g was used in the definition of the covariant derivative, it stands to reason that
                                   it would be invariant only under those reparametrization which preserve the metric, i.e., under
                                   isometries.
                                                                                
                                                                                              
                                   Proposition 3. Let   : U,g        (U,g)  be an isometry. Let  Y T U,  u      and let  Z  be a vector field on
                                   U.  Then
                                   
                                                                                .
                                                                   
                                                               d     Y Z    d Y    d Z         ...(12)
                                                                             
                                                                          
                                   Proof. This proof, although tedious, is quite straightforward, and is relegated to the exercises.
                                                                                        
                                   Note that on the left hand-side of (12), the covariant derivative    is that obtained from the
                                   metric  g. 
                                   Our next observation, which follows almost immediately, gives an interpretation of the covariant
                                   derivative when the metric g is induced by a parametric surface X.
                                   Proposition 4. Let the Riemannian metric g be induced by the parametric surface X. Then the
                                                                         
                                   image under dX of the covariant derivative  dX  i   Z  is the projection of   i Z  onto the tangent
                                   space.

                                                    
                                                                     j
                                   Proof. Note that  dX    X .  Thus, if  Z   z  j  then we find:
                                                    i
                                                         i
                                                              j
                                                                                   j
                                                                            k
                                                    dX  i Z    z X   z X   ik j  z X   i  z X j  k z N,  ij  j
                                                                    j
                                                                    ;i
                                                                              j
                                                                j
                                                                      j
                                                              ;i
                                   which proves the proposition.
                                   We now show that covariant differentiation is in addition well-adapted to the metric g.
                                   Proposition 5. Let (U, g) be a Riemannian surface, and let Y and Z be vector fields on U. Then, we
                                   have
                                                                ig (Y,Z)    g  i Y,Z  g   i Y,Z .  ...(13)
                                   Proof. We  first note  that, as  in the  proof of  Theorem 2.29,  the definition  of the  Christoffel
                                   symbols (3) :
                                                               g ij,l    k il g   k jl g .            ...(14)
                                                                       kj
                                                                            ki





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