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math214:04-15 [2020/04/15 00:29]
pzhou
math214:04-15 [2020/04/15 00:55] (current)
pzhou
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 ====== 2020-04-15, Wednesday ====== ====== 2020-04-15, Wednesday ======
  
-==== Cartan's Moving Frame ====+===== Cartan's Moving Frame =====
 Pick any **Orthonormal Frame ** $X_\alpha$ of $TM$, and choose its dual frame $\theta^\alpha$ of $T^*M$. Introduce a collection of 1-forms using covariant derivatives  Pick any **Orthonormal Frame ** $X_\alpha$ of $TM$, and choose its dual frame $\theta^\alpha$ of $T^*M$. Introduce a collection of 1-forms using covariant derivatives 
 $$ \nabla X_\alpha = \omega_\alpha^\beta X_\beta $$ $$ \nabla X_\alpha = \omega_\alpha^\beta X_\beta $$
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 $$X_i = \frac{1}{h_i} \d_{x^i}, \theta^i = h_i dx^i $$ $$X_i = \frac{1}{h_i} \d_{x^i}, \theta^i = h_i dx^i $$
 Then, we can get $\omega_i^j$ by solving Then, we can get $\omega_i^j$ by solving
-$$ d \theta^i = -\d_j(h_i) dx^i \wedge dx^j $$+$$ d \theta^i = d(h_i) \wedge dx^i $$ 
 +Now, one need to figure out what is $\omega_i^j$ in each specific cases. Once that is done, one can easily get the curvature.  
 + 
 + 
 +===== Aside: Ehresmann connection, Connection on Principal Bundle ===== 
 +Another more geometric notion of connection is called Ehresmann connection, it applies to fiber bundle. Let $\pi: E \to M$ be a fiber bundle. A connection is a splitting of  
 +$$T_p E = T_p E_h \oplus T_p E_v $$ 
 +where $h$ stands for horizontal and $v$ for vertical. $TE_v$ is canonical, it is the tangent space to the fiber. $T_p E_h$ contains information.  
 + 
 +If $P$ is a principal $G$-bundle, then we want the choice of horizontal subspace to be invariant under the (right) action of $G$.  
 + 
 +Parallel transport along a path $\gamma: [0,1] \to M$ on $M$ gives a diffeomorphism 
 +$$ P_\gamma: E_{\gamma(0)} \to E_{\gamma(1)}. $$ 
 +In the case of $G$-bundle, this diffeomorphism commute with the right $G$-action on the fiber.  
 + 
 +If $V$ is a represenation of $G$, we may form the associated bundle $P \times_G V$, where each fiber over $b \in M$ is $$ P_b \times_G V = \{ (p , v) \in P_b \times V \} / (p g, v) \sim (p, g \cdot v) \cong V $$ 
 +since $G$ acts on $P_b$ freely and transitively ($P_b$ is said to be a $G$-torsor). Then, $P_\gamma$ also induces parallel transport on $P \times_G V$.  
  
  
math214/04-15.1586935776.txt.gz · Last modified: 2020/04/15 00:29 by pzhou