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Let $E\to N$ be a vector bundle and $f:M\to N$ be a smooth map. The pullback $f^*:\Omega^k(N,E)\to \Omega^k(M,f^*E)$ is then defined by $$(f^*\omega)_x(v_1,...,v_k)=\omega_{f(x)}((df)_x(v_1),...,(df)_x(v_k))$$ with $x\in M$ and $v_1,...,v_k\in T_xM$.

First question: how can I rewrite this pullback as a map $f^*\omega:\mathfrak{X}(M)\times...\times \mathfrak{X}(M)\to \Gamma(M,f^*E)$? My problem is that $df:\mathfrak{X}(M)\to \mathfrak{X}(N)$ is well defined as long as $f$ is a diffeomorphism. However, $df:\mathfrak{X}(M)\to \Gamma(M,f^*TN)$ is actually well defined.

Then, I know that the connection $f^*\nabla$ on $f^*E\to M$ is uniquely determined by $$(f^*\nabla)(f^*s):=f^*(\nabla(s))\in \Omega^1(M,f^*E)$$

Second question: In some books, I saw the notation $$(f^*\nabla)_X(f^*s)=f^*(\nabla_{df(X)}(s))=\nabla_{df(X)}(s)\circ f$$ but as long as $f$ is not a diffeomorphism $df(X)$ is not a vector field on $N$ so it doesn't make sense writing $\nabla_{df(X)}$. How can I solve this problem?

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  • $\begingroup$ Why are you trying to give a map $\mathfrak X(M)\to\mathfrak X(N)$? Don't you just need a vector field along the image of $M$? I don't understand what $f^*(\nabla s)$ means. A section of $f^*E$ is not the same as the pullback of a section of $E\to N$, is it? $\endgroup$ Oct 18, 2020 at 22:51
  • $\begingroup$ If I want to write the pullback as $f^*\omega(X_1,...,X_k)=(\omega\circ f)(df(X_1),...,df(X_k))$, I need $df:\mathfrak{X}(M)\to \mathfrak{X}(N)$ to be well defined, right? $\nabla:\Gamma(N,E)\to \Omega^1(N,E)$, so $f^*(\nabla(s))$ is the pullback of the 1-form $\nabla(s)$ $\endgroup$
    – Watanabe
    Oct 19, 2020 at 9:43
  • $\begingroup$ There is also another induced map from the sections of $E\to N$ to the sections of $f^*E\to M$, $f^*:\Gamma(N,E)\to \Gamma(M,f^*E)$ given by precomposition. $\endgroup$
    – Watanabe
    Oct 19, 2020 at 9:53

1 Answer 1

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To write the pullback globally as a map of modules, you need to split the construction into two parts. To make everything less confusing, let me denote by $f^{\star}(E)$ the pullback bundle and denote by $\mathfrak{X}_f(M) = \Gamma(M,f^{\star}(TN))$ vector fields along $f$. Thus, the maps and constructions involving $\star$ have nothing to do with the derivative while the maps involving $*$ include the derivative. Now,

  1. Given a form $\omega \in \Omega^k(N,E)$, we get an element $f^{\star}(\omega) \in \Gamma \left( \operatorname{Alt}^k \left( f^{\star}(TN), f^{\star}(E)\right) \right)$ given by $$ f^{\star}(\omega)|_p \left( \xi_1, \dots, \xi_k \right) = \omega_{f(p)} \left( \xi_1, \dots, \xi_k \right)$$ where $\xi_i \in \mathfrak{X}_f(M)$ are vector fields along $f$ so that $\xi_i(p) \in T_{f(p)}N$ and the formula makes sense. Globally, this corresponds to an alternating map of $C^{\infty}(M)$-modules $$f^{\star}(\omega) \colon \mathfrak{X}_f(M) \times \dots \mathfrak{X}_f(M) \rightarrow \Gamma(f^{\star}(E)).$$
  2. In addition, you have the map $df \colon \mathfrak{X}(M) \rightarrow \mathfrak{X}_f(M)$. Then $$ f^{*}(\omega)(X_1, \dots, X_k) = f^{\star}(\omega)(df(X_1), \dots, df(X_k)). $$

Regarding the second question, the formula $$ f^{*}(\nabla)_{X}(f^{\star}(s)) = \nabla_{df(X)}(s) \circ f $$ is meant to be understood locally as $$ \left( f^{*}(\nabla)_{X}(f^{\star}(s)) \right)|_{p} = \left( \nabla_{df|_{p}(X)}(s) \right) \textrm{ (at }f(p)\textrm{)}.$$ It makes sense even when $f$ is not a diffeomorphism as a connection $\nabla_X(s)$ is tensorial in the $X$ variable. You can also understand the formula globally by splitting the construction of the pullback connection into two parts:

  1. There is a map $f^{\star}(\nabla) \colon \mathfrak{X}_f(M) \times \Gamma(E) \rightarrow \Gamma(f^{\star}(E))$ given by $$ \left( f^{\star}(\nabla)_{\xi} \right)(s)|_{p} = \left( \nabla_{\xi(p)} s \right)|_{f(p)}. $$
  2. The pullback connection $f^{*}(\nabla)$ is the unique connection $f^{*}(\nabla) \colon \mathfrak{X}(M) \times \Gamma(f^{\star}(E)) \rightarrow \Gamma(f^{\star}(E))$ which satisfies $$ f^{*}(\nabla)_{X}(f^{\star}(s)) = f^{\star}(\nabla)_{df(X)}(s). $$
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