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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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